To investigate the effect of the ionic liquid (IL) chain length on the surface properties and photoactivity of TiO2, a series of TiO2 microspheres have been synthesized via a solvothermal method assisted by 1-methyl-3-octadecylimidazolium chloride ([ODMIM][Cl]) and 1-methyl-3-tetradecylimidazolium chloride ([TDMIM][Cl]). All as-prepared samples were characterized by X-ray powder diffraction (XRD), X-ray photoelectron spectroscopy (XPS), diffuse reflectance spectroscopy (DRS), scanning transmission microscopy (STEM) and the Brunauer–Emmett–Teller (BET) surface area method, whereas the photocatalytic activity was evaluated by the degradation of phenol in aqueous solution under visible light irradiation (λ > 420 nm). The highest photoefficiency (four times higher than pristine TiO2) was observed for the TiO2 sample obtained in the presence of [TDMIM][Cl] for a IL to TiO2 precursor molar ratio of 1:3. It was revealed that interactions between the ions of the ionic liquid and the surface of the growing titanium dioxide spheres results in a red-shift of absorption edge for the IL–TiO2 semiconductors. In this regard, the direct increase of the photoactivity of IL–TiO2 in comparison to pristine TiO2 was observed. The active species trapping experiments indicated that O2•− is the main active species, created at the surface of the IL–TiO2 material under visible-light illumination, and is responsible for the effective phenol degradation.
The development of heterogeneous photocatalysis to degrade organic pollutants in aqueous and gas phases requires visible-light responsive, stable materials and a basic understanding of these materials [1-4]. Although various semiconductors are considered for environmental pollution abatement, titanium dioxide (TiO2) is still the most promising due to its stability, low cost, nontoxicity and availability . Despite many advantages, the commercial application of TiO2 to solve environmental problems is still limited. The main obstacle is the relatively wide band gap of 3.2 eV for anatase that limits the photoexcitation wavelength needed to activate photocatalytic reactions to ultraviolet (UV) irradiation . To break through the aforementioned drawbacks, semiconductor coupling , sensitization by inorganic complexes or organic dyes [8,9], as well as metal nanoparticle (NP) deposition  and metal doping  have been applied and have revealed potential to achieve visible-light-activated photocatalysts.
Another, actually surprising, way to improve the efficiency of solar-driven photocatalysis appeared in an application of ionic liquids (ILs) for TiO2 preparation [12-14]. Sometimes referred to as “solvents of the future”, ILs have induced a large and still growing interest from the scientific community and continuously find new areas of application. This scientific interest comes from the many interesting properties such as negligible vapor pressure, high thermal and electrochemical stability, and inflammability, providing a neoteric media for nano- and microstructure preparation with novel properties . Especially, their polarity and affinity towards particles and precursors, transport and surface properties seem to be crucial for formation of the protective layer at the particle surface, thus electrosteric, solvation and viscous stabilization of growing particles [15-18].
The initial works on the application of ILs for semiconductor (including TiO2) preparation were focused mainly on the usage of these salts as solvents (reaction medium) [19-21] or components of the reaction system [22-25]. Their role was devoted to control the crystallization process and formation of the final particle structure (structuring agent). In this regard, various interesting structures were obtained and their properties are described in the literature. However, the more advanced works presented examples of the practical usage of the IL–TiO2 composites, for example, for photo-electrochemical water splitting [26,27], photo-oxidation of benzyl alcohol , phenol , degradation of chlorophenol [17,29], reduction of Cr6+ to Cr3+ and the photocatalytic desulfurization of diesel oil . Nevertheless, in most of these publications the photoactivity of TiO2 was determined under UV–vis irradiation [17,26,27,29,31-35]. Much less attention, in contrast, has been paid towards the enhancement of the visible light photoactivity of TiO2 by ILs and the elucidation of the role of ILs in the mode of action of photocatalysts [12,13,36-38]. Interestingly, in all mentioned publications [12,13,36-38] the same ionic liquid, 1-butyl-3-methylimidazolium tetrafluoroborate ([BMIM][BF4]), was used. However, the proposed mechanisms were different. The photoactivity enhancement under visible-light irradiation was proposed to be due to: (i) doping of nonmetal elements (e.g., N, B, F) derived from the IL structure, inducing a narrower band gap and improving the separation efficiency of the photogenerated electron/hole pairs [13,36,37]; (ii) enhancement of Ti3+ species formation in the TiO2 lattice (being a source of the electronic charge required for O2 adsorption and intermediate energy level) [12,36]; (iii) promoting TiO2 hollow structure formation, thereby shortening the diffusion length of the charge carriers as well as increasing the number of reactive sites ; and (iv) direct sensitization of TiO2 photocatalysts . The only exception is our previous work , where three ILs composed of 1-butyl-3-methylimidazolium cation [BMIM] and bromide, hexafluorophosphate [PF6] and octylsulphate [OctSO4] anions were used. In contrast to [BMIM][BF4], the improved TiO2 photoactivity under visible-light irradiation originated from the interaction of the bromide anion and molecular oxygen with the TiO2 surface with formation of surface complex . Therefore, taking into account the ease of modification of the cation and anion structure of the IL, and as a consequence, the altering of their physicochemical properties, the mechanism of the visible-light activity improvement may vary depending on the IL composition. However, the relation between the IL structure and visible-light photoactivity as well as its mode of action is still not known.
In this regard, in this comparative study, we have continued the elucidation of the role of the IL (alkyl chain length in the imidazolium cation) as well as the effect of the IL structure on the formation of TiO2 photocatalysts with improved activity towards visible irradiation. The structures of the ILs used in this study, 1-methyl-3-tetradecylimidazolium ([TDMIM][Cl]) and 1-methyl-3-octadecylimidazolium chlorides ([ODMIM][Cl]), are shown in Figure 1. This study gave us better phenomenological insight into the performance of the IL–TiO2 photocatalysts and better prospects for optimizing the IL of choice. The results form a part of a very broad, but hardly touched issue in the field of IL–TiO2 composites, that is, which structural descriptors of ILs are crucial for the preparation of visible-light-active photocatalysts with desired morphology and properties and how to predict the properties of the IL–TiO2 material on the basis of the structure and properties of IL.
Results and Discussion
Twelve novel TiO2 photocatalysts prepared in the presence of two ionic liquids containing different alkyl chain lengths in the imidazolium cation ([ODMIM][Cl] and [TDMIM][Cl]) were obtained by the solvothermal method. All samples were prepared in six different molar ratios IL:TBOT (see Table 1). First of all, the samples were analyzed in terms of specific surface area, optical and photocatalytic properties (in a model reaction of phenol degradation in the aqueous phase under visible-light irradiation). The description of all prepared photocatalysts, including the selected physicochemical and photocatalytic properties, is shown in Table 1. To understand the nature of the visible-light-induced activity (IL:TBOT molar ratio equal to 1:3 and 1:10), the photocatalysts possessing the highest and lowest activity have been selected for further detailed study (SEM, XPS and XRD). Moreover, for the two samples with the highest photoactivity (TiO2_T(1:3) and TiO2_O(1:3)), the active species involved in the photocatalytic reaction were also determined.
Specific surface area (SBET), pore volume and the efficiency of phenol degradation after 60 min visible-light irradiation of the samples tested in this study.
Molar ratio (IL:TBOT)
Specific surface area (m2·g−1)
Efficiency of phenol degradation (%)
Morphology and phase structure
The crystal structure of the selected IL–TiO2 samples was characterized by XRD, as shown in Figure 2. The typical diffraction peaks corresponding to anatase phase of TiO2 (2θ = 25.3°, 37.8°, 48.1°, 54°, 54.9°, 62.7°, 68.5°, 70.2°, 75°, 82.6°) were observed for all photocatalysts. The analysis confirmed that the samples do not contain any impurities and anatase phase of high quality was formed. Based on the line width analysis of the anatase (101) reflection peak, the average crystal size of the crystallites (d) forming photocatalysts with the highest (IL:TBOT molar ratio 1:3) and the lowest photoactivity (IL:TBOT molar ratio 1:10), estimated by the Scherrer equation, were determined and summarized in Table 2.
Lattice parameters and average crystallite size of the IL–TiO2 photocatalysts. The values in parenthesis represent the error in measurement.
The average crystal size values of the IL–TiO2 composites generally increased with the addition of ILs in comparison to pristine TiO2. This could suggest that the addition of ILs during the preparation of TiO2 affects the growth of the anatase nanocrystals, forming microparticles. Similar results were reported by Li et al.  who suggest that [BMIM][BF4] acted as a growth inhibitor of the anatase crystal. The addition of ILs to the TiO2 preparation route also influenced the length of the cell edges – a decrease of a and increase of c lengths in comparison to pristine TiO2 was detected. These observations can be related to changes in the crystalline structure, i.e., generation of Ti3+ as will be described below in the next section. Comparing the IL–TiO2 samples, the photocatalysts with the highest activity were characterized by the shorter length of both cell edges as well as the lowest cell volume (Table 2).
The surface morphology and microstructure of the IL–TiO2 composites were characterized by SEM. The morphology of four selected samples prepared with different IL concentrations (IL:TBOT molar ratio equal to 1:3 and 1:10) which revealed the highest and the lowest photoactivity under visible-light irradiation is presented in Figure 3. The average size of the microspheres, calculated based on the statistical average size of 100 microstructures, is also included in this figure. The four main fractions of TiO2 microspheres have been recognized. Generally, for all the samples, the dominant fraction were the microspheres with an average diameter ranging from 3 to 5 µm. Based on these results, as well as our previous study , we can conclude that longer alkyl chains in the imidazolium cation lead to a larger particle size. Recently we examined the influence of two ionic liquids with four and ten atoms of carbon in the alkyl chain of the imidazolium cation (i.e., 1-butyl- and 1-decyl-3-methylimizadolium chlorides, [BMIM][Cl] and [DMIM][Cl], respectively) on the selected properties and photoactivity of TiO2 particles under UV irradiation. For [BMIM][Cl] (IL:TBOT molar ratio 1:10), the highest contribution (44%) had structures with diameter 0.5–1 μm, whereas for [DMIM][Cl], up to 50% were particles of 1–2 μm. For comparison, IL–TiO2 structures prepared in this study in the presence of [TDMIM][Cl] and [ODMIM][Cl], for a IL:TBOT molar ratio equal to 1:10, yielded mainly particles with a diameter of 3–5 μm, in an amount of 54% and 49%, respectively. It was also observed that synthesis in the presence of low IL content in the reaction mixture (i.e., IL:TBOT molar ratio of 1:10) provided TiO2 structures with deformations (Figure 3), whereas the photocatalysts prepared using a IL:TBOT molar ratio equal to 1:3 (TiO2_T(1:3) and TiO2_O(1:3)) had a more uniform, spherical shape and smoother surface. Moreover, increasing the concentration of IL resulted in formation of particles with a higher contribution of smaller particles in comparison to samples obtained using IL:TBOT with a molar ratio equal to 1:10. [TDMIM][Cl] and [ODMIM][Cl] are salts consisting of a large, asymmetric, amphiphilic imidazolium cation and a small single-atomic chloride anion. Based on our previous research we can assume that ILs interact with the TiO2 surface, making a protective layer due to a combination of electrostatic and steric stabilization. 1-Methyl-3-octadecylimidazolium chloride is probably less firmly packed on the TiO2 surface due to the longer alkyl chain. As a result, the [ODMIM][Cl] ionic liquid may limit smaller particle deposition during Ostwald ripening, thus inhibiting further growth and agglomeration. For the TiO2_O(1:3) sample, the dominant fraction were microspheres with diameter ranging from 2–3 μm (38%), whereas for TiO2_T(1:3), the main fraction was particles with an average diameter of 3–5 μm (42%).
Diffuse reflectance spectroscopy, UV–vis spectroscopy and BET analysis
The Brunauer–Emmett–Teller (BET) specific surface area (SBET) of the IL–TiO2 photocatalysts ranged from 119 to 211 m2·g−1 (see Table 1). For comparison, pristine TiO2 obtained by the same method but without IL, has a SBET equal to 199 m2·g−1. In this regard, all samples (except TiO2_T(1:10) ) had a smaller SBET as compared to TiO2 unmodified by ILs. Taking into account the type and the amount of IL used in the experiments, the largest SBET was detected for the IL–TiO2 samples obtained with the IL:TBOT molar ratio of 1:10, that is, the lowest amount of IL used for TiO2 synthesis. The specific surface area determined for these samples was 211 m2·g−1 and 193 m2·g−1 for [TDMIM][Cl] and [ODMIM][Cl], respectively. Further increase of the IL content in the reaction mixture resulted in decrease of SBET. The results obtained for both IL are similar (Table 1), therefore influence of the chain length in the imidazolium cation on the surface properties of IL–TiO2 was not observed. However, the comparison of SBET of samples described in this work with values previously presented by Paszkiewicz  for ILs containing shorter chain lengths in the imidazolium cation (C4 and C10) revealed that elongation of the alkyl substituent provided photocatalysts with smaller surface area. This property may be related to formation of the protecting layer by the IL at the TiO2 surface, resulting therefore in higher steric hindrance for salts with longer alkyl chains influencing the final pore volume, and thus, the surface area. The total pore volume ranged from 0.05 to 0.1 cm3·g−1 depending on the IL type used in the experiments and its concentration. A higher BET surface area was also related to higher pore volume values and could lead to improved efficiency of the photocatalytic reactions .
The diffuse reflection (DR)/UV–vis spectra of the photocatalysts as well as for the pure ionic liquids used in this study are shown in Figure 4. The pristine TiO2 obtained by the solvothermal method showed the expected bandgap of 3.2 eV and very weak visible-light absorption. However, the visible-light absorption of the TiO2 photocatalysts appeared when the selected ionic liquids, [ODMIM][Cl] and [TDMIM][Cl], were applied in the TiO2 synthesis reaction. Moreover, with increasing IL:TBOT molar ratio, the optical absorption of the composites in the viible-light region was also greatly increased (compare for example spectra for IL–TiO2 obtained at IL:TBOT molar ratio of 1:10 and 1:3). Therefore, this enhanced absorbance of the light in the visible spectrum is expected to enhance the photocatalytic activity in the visible region for the target reaction. This observation is well verified by the photocatalytic tests of the IL–TiO2 composites for the phenol degradation under visible light irradiation (Table 1).
Additionally, to understand why the obtained microparticles exhibited a strong light absorption over the visible range pure ILs were also examined as shown in Figure 4. The shape and nature of the imidazolium ionic liquid spectra are consistent with literature data [40,41]. A clear maximum is observable above 220 nm and a long tail of the absorption extended even beyond 350 nm and 500 nm for [ODMIM][Cl] and [TDMIM][Cl], respectively. The intense absorption in the UV region can be assigned to the π–π* transition of the imidazolium ring. On the other hand, the long tail of the absorption spectra could be due to (i) the energy structure of the cation as well as the spatial arrangement of the anion and (ii) the presence of an impurity resulting from the IL synthesis [42-44].
Considering the above results the improvement of the optical absorption of the composites in the visible-light region could be associated with the synergic effect of its two main components, that is, TiO2 and ILs. Binetti et al.  stated that the absorbance of IL–TiO2 materials increased with the modification of TiO2 with 1-hexyl-3-methylimidazolium tetrafluoroborate ([HMIM][BF4]), and concomitantly, a tail appears in the visible region due to absorption by IL. Moreover, taking into account that both ILs used in this study have a high number of carbon atoms in the structure (Figure 1), thus high carbon content, the absorption of IL–TiO2 in the visible region can be attributed to the existence of carbon species on the surface of the photocatalysts .
Chemical composition of ionic liquid/TiO2 composites
The photocatalytic degradation is based on chemical reactions on the surface of the photocatalyst [46-48]. In this context, XPS measurements have been chosen to analyze the surface of the IL–TiO2 composites. Both [ODMIM][Cl]–TiO2 and [TDMIM][Cl]–TiO2 samples modified with a IL:TBOT molar ratio of 1:3 and 1:10 were investigated. The elemental surface composition of all IL–TiO2 specimens analyzed is shown in Table 3. The titanium, oxygen, carbon, nitrogen and chlorine atoms were detected. The last two elements evidenced successful interaction between the IL and the surface of TiO2. The chemical character of these elements was identified from corresponding Ti 2p, O 1s, C 1s, N 1s and Cl 2p high-resolution XPS spectra, respectively. The deconvoluted spectra are shown in Figure 5. The carbon fraction at binding energy (BE) close to 286.2 eV is characteristic for C–Cl and C–N bonds . Two nitrogen states can be distinguished in the N 1s spectra recorded on the IL–TiO2 composites (see Figure 5 and Table 3). The signal at BE = 400 eV can be assigned to nitrogen states formed by Ti–O–N and C–N bonds . The last one can be from superposition of C–NH–C and C=N–C bonds attributed to pyrrole- and pyridine-type interactions [49,51,52]. The peaks at BEs above 401.4 eV can be due to the positively charged nitrogen (N+) caused by pyridine-type nitrogen bonds and oxidized nitrogen species . It should be noted that this nitrogen state appears for both types of IL–TiO2 with a molar ratio of IL:TBOT of 1:3. No signals located at BEs lower than 399 eV, characteristic for Ti–N bond formation , were detected. The XPS data collected in Table 3 showed that the amount of carbon, nitrogen and chlorine were higher for the samples with molar ratio 1:3 than for those with molar ratio 1:10. In addition, the surface concentration of these elements for the TiO2_O(1:3) sample with longer alkyl substituents is smaller than corresponding values evaluated for TiO2_T(1:3) samples containing ILs with shorter substituents (see the C/Ti and N/Ti entries in Table 3). Thus, the lower coverage of the [ODMIM] cations seems to be the result of the larger steric effect induced by this ion. The C/N ratios, evaluated for all samples, were estimated to be higher than nominal values related to the respective IL cations (see Table 3). This may be caused by adsorption of additional carbon contaminants on the finally prepared IL-assisted TiO2 because of the exposure of the samples to air prior to the XPS analysis or during synthesis and preparation.
Elemental composition (in atom %) and chemical characteristics of titanium, oxygen, carbon and nitrogen states in the surface layer of [ODMM][Cl] and [TDMM][Cl] IL-modified TiO2 particles, evaluated by X-ray photoelectron analysis.
Ti(4+) 458.9 ± 0.2 eV
Ti(3+) 457.2 ± 0.2 eV
Ti–Olatt 530.0 ± 0.1 eV
Ti–Osurf 530.6 ± 0.2 eV
C=O 531.6 ± 0.2 eV
–OH 532.6 ± 0.2 eV
C–C 284.8 ± 0.1 eV
C–OH, C–Cl, C–N 286.2 ± 0.1 eV
–C=O, N–C=O 289.0 ± 0.1 eV
“A” 400.0 ± 0.4 eV
“B” 401.4 ± 0.1 eV
The photocatalytic activity of the IL–TiO2 samples was evaluated by phenol degradation induced by visible-light irradiation (using an optical filter with λ > 420 nm). All photocatalysts exhibited better photocatalytic properties than the reference TiO2 sample (Table 1 and Figure 6).
Before the photocatalytic activity tests, phenol adsorption on the surface of the photocatalyst was tested for the samples possessing the highest photoactivity. It was observed that the concentration of phenol after 120 min in dark conditions practically did not change. The samples with the highest photoactivity were prepared using a IL:TBOT molar ratio of 1:3. The efficiency of phenol degradation increased from 14 to 59% and 61% for pristine TiO2, TiO2_O(1:3) and TiO2_T(1:3) samples, respectively. Moreover, for both ionic liquids the phenol degradation efficiency increased with increasing IL:TBOT molar ratio from 1:10 to 1:3. However, a further increase in the IL concentration in the reaction system resulted in an opposite relation. These results corresponded well with SEM and XRD results. Particles prepared using a IL:TBOT molar ratio equal to 1:10 were poorly formed and had highly irregular shapes, which resulted in lower photocatalytic activity. Based on the literature data, it is known that regularly shaped TiO2 microspheres show a higher photoefficiency due to their low density, high surface-to-volume ratio, high surface area and good surface permeability [54-56]. Thus, it could be expected that the higher photocatalytic activity could be achieved by using TiO2 microspheres with uniform and spherical shape.
According to the DRS UV–vis spectra shown in Figure 4, the incorporation of ILs into TiO2 microspheres significantly extended the absorption spectrum of the titanium dioxide in the visible region. Therefore, the enhanced photocatalytic activity of IL–TiO2 can be attributed to the improved optical absorption. Moreover, the XPS data showed that the amount of carbon, nitrogen and chlorine were higher for the samples with molar ratio 1:3 in comparison to 1:10, which corresponds well with changes in photoactivity. It should be noticed that the total amount of C, N and Cl was higher for TiO2_T(1:3) than TiO2_O(1:3) despite that the [ODMIM] cation contained a longer alkyl chain than [TDMIM]. This is probably due to the higher steric hindrance created by [ODMIM][Cl] at the TiO2 surface, hence a probably less firmly packed organic protection layer. Additionally, the XPS analysis also confirmed that C, N and Cl atoms are located solely on the surface of the semiconductors. Hereby, the possible mechanism of the TiO2 photoactivity improvement under visible-light irradiation by doping of nonmetal elements derived from IL structures was rejected.
Therefore, to further elucidate the mechanisms of the photocatalytic reaction, the role of the generated reactive species in the photocatalytic process under visible irradiation was investigate using t-BuOH, AgNO3, p-benzoquinone (BQ) and ammonium oxalate (AO) as the scavengers of •OH, e−, O2−• and h+, respectively. These measurements have been performed for the IL–TiO2 samples possessing the highest activity, that is, TiO2_T(1:3) and TiO2_O(1:3), and the obtained results are presented in Table 4. It was observed that application of AgNO3 as a scavenger of e− for the both samples (TiO2_T(1:3) and TiO2_O(1:3) did not affect the effectiveness of the photocatalytic process compared to that carried out without scavengers.
Percent efficiency of phenol degradation under visible light in the presence of scavengers.
Participation of O2• in the photodegradation process was investigated by adding BQ, which is capable of trapping O2•. It was observed that the addition of BQ to both samples (TiO2_O(1:3) and TiO2_O(1:3)) caused inhibition of phenol degradation, as presented in Table 4. The degradation rate was largely suppressed to 22 and 11% for the TiO2_T(1:3) and TiO2_O(1:3) photocatalysts, respectively. It is deduced that the oxidation inhibition of phenol is due to the suppression of the superoxide anion formation by the BQ addition. Addition of AO (holes scavenger) resulted in a slight inhibition of the photodegradation process under visible-light irradiation for both samples, indicating that h+ might play a negligible role in the phenol photo-oxidation process. Probably the positively charged hole could catch OH− to yield hydroxyl radicals . In the case of the TiO2_T(1:3) sample, when tert-butyl alcohol (•OH scavenger) was added to the phenol solution, 63% of phenol was degraded, indicating that OH radicals play an insignificant role in the degradation process. Interestingly, for the TiO2_O(1:3) photocatalyst, the addition of AgNO3 and tert-butyl alcohol increased the effectiveness of the photocatalytic process. As explained by Liu et al., AgNO3 may be capable of enhancing the separation of electrons and holes, resulting in a greater amount of holes and following active species generated, which promotes the degradation rate .
The results presented in this study revealed that visible-light-responsive TiO2 microspheres could be successfully obtained by a solvothermal method assisted by ionic liquids, such as 1-methyl-3-tetradecylimidazolium or 1-methyl-3-octadecylimidazolium chlorides. The ionic liquids introduced into the reaction environment work as structure-controlling agents, providing TiO2 microparticles (composed of nanocrystals) with a large specific surface area ranging from 119 to 211 m2/g. However, more importantly, application of ionic liquids during TiO2 synthesis enabled formation of visible-light-induced photocatalysts. It was found that the amount of the ionic liquid used for the synthesis is crucial and significantly affects the photoresponse of the IL–TiO2 materials toward visible irradiation, thus photoactivity. The highest photoactivity was observed for samples prepared using a IL:TBOT molar ratio of 1:3, as observed for both ILs. From 59% to 61% of phenol used as a model compound was degraded after 60 min of irradiation by visible light (λ > 420 nm) in the presence of suspended TiO2 that was modified by [ODMIM][Cl] and [TDMIM][Cl], respectively. The enhanced photocatalytic activity of IL–TiO2 can be attributed to the presence of the ionic liquid cation and anion at the TiO2 surface, resulting in the improved optical absorption of visible light by the photocatalysts. The phenol degradation was realized mainly by radical anions O2•−, whereas the contribution of the other active species was limited in the reaction mechanism. In this regard, the role of the ionic liquid in TiO2 photoexcitation requires further investigation.
Titanium(IV) n-butoxide (TBOT), (≥97%) as a precursor of TiO2, hydrochloric acid (36%) as a pH stabilizer and ethanol (99.9%) as the reaction medium were provided by Sigma-Aldrich. The ionic liquids, 1-methyl-3-octadecylimidazolium chloride [ODMIM][Cl] and 1-methyl-3-tetradecylimidazolium chloride [TDMIM][Cl] were purchased from Ionic Liquids Technologies GmbH. Ammonium oxalate, silver nitrate (≥99%), benzoquinone and tert-butyl alcohol from Sigma-Aldrich were used as scavengers.
TiO2 was modified by ILs using a solvothermal method. First of all, the titania precursor, Ti(IV) n-butoxide, was dissolved in absolute ethanol under stirring. Then the hydrochloric acid, distilled water and selected ionic liquid were added. Vigorous stirring of the solution was continued for 10 min to obtain a transparent solution. In the final step, the homogeneous mixture was transferred to a 200 mL teflon-lined stainless steel autoclave and the solvothermal reaction was performed at 180 °C for 24 h . The reaction product was washed with ethanol and deionized water, respectively, followed by drying at 60 °C for 6 h. The obtained powder was calcinated at 200 °C for 2 h (heating rate 2 °C/min). Various molar ratios of ILs to TBOT were selected as listed in Table 1.
The morphology and size distribution of the TiO2 powders were observed using a Jeol SEM microscope operated at 12 kV and Cs-corrected STEM (high angle annular darkfield, HAADF).
X-ray photoelectron spectroscopy (XPS) experiments were performed on a PHI 5000 VersaProbeTM (ULVAC-PHI) spectrometer with monochromatic Al Kα radiation (hν = 1486.6 eV). The high-resolution (HR) XPS spectra were collected by the hemispherical analyzer at a pass energy of 23.5 eV and an energy step size of 0.1 eV. CasaXPS software was used to evaluate the XPS data. The binding energy (BE) scale of all detected spectra was referenced by setting the BE of the aliphatic carbon peak (C–C) signal to 284.8 eV.
The UV–vis reflectance and absorbance spectra of TiO2 photocatalysts were recorded using a Shimadzu UV–vis spectrophotometer (UV 2600) equipped with an integrating sphere and BaSO4 was used as the reference sample.
BET surface area and total pore volume of the photocatalysts (physical adsorption and desorption of nitrogen at 77 K) was measured using a Micromeritics Gemini V200 instrument. The photocatalyst samples were dried and degassed in a sample cell at 200 °C for at least 2 h before the adsorption. The specific surface area of the photocatalysts was determined by the BET method.
Powder X-ray diffraction (XRD) studies of the photocatalyst samples were carried out using a RigakuMiniFlex 600 XRD system equipped an X-ray generator with a copper target (operated at 40 kV and 30 mA). The average TiO2 crystallite size was calculated using the Scherrer equation.
Photocatalytic activity test
For determination of the photoactivity under visible-light irradiation, the aqueous phase containing 125 mg of the photocatalyst (5 g/dm3), 24 cm3 of deionized water and 1 cm3 of phenol as a model compound (Co = 500 mg/dm3) was used. The suspension was stirred and aerated (V = 5 dm3/h) for 30 min in the dark to obtain equilibrium and then the content of the reactor was photoirradiated with a 1000 W Xe lamp (Oriel, light flux 6.5–7.5 mW/cm2) which emitted both UV and visible-light irradiation. The photoreactor (V = 25 cm3, i.d. 37 mm, length 30 mm) was equipped with a quartz window and exposure layer thickness was 3 cm. The optical path included a water filter and a glass filter (GG 420) which cut-off wavelengths shorter than 420 nm. The temperature of the aqueous phase during irradiation was kept at 10 °C using a water bath. During the irradiation, the suspension (1 cm3) was collected and filtered through syringe filters (diameter 0.2 µm) to remove the photocatalyst particles. The phenol concentration was estimated by means of the colorimetric method (λ = 480 nm) after derivatization with diazo-p-nitroaniline using a UV–vis spectrophotometer (Thermo Evolution 220). The photocatalytic degradation runs were preceded by a blind test in the absence of a photocatalyst or illumination. No degradation of phenol was observed in the absence of either the photocatalyst or illumination.
Determination of reactive species
To clarify which active species are involved in the photodegradation of the model compound, the phenol irradiation process was preceded by analogous experiments performed in the presence of different radicals scavengers (ammonium oxalate as a scavenger for photogenerated holes, AgNO3 as scavenger for electrons, benzoquinone (BQ) as scavenger for superoxide radical species, and tert-butyl alcohol as a scavenger for hydroxyl radical species). The procedure of the photocatalytic measurements was carried out similar to the above-described photocatalytic degradation of phenol, except that the radical scavengers were added to the reaction system. The scavenger concentration was equal to 0.21 mmol dm−3. No adsorption of phenol was observed in the presence of the photocatalyst in the phenol/scavenger solution and absence of illumination.
The authors acknowledge funding from the National Science Center within the program SONATA 8, research grant: “Influence of the ionic liquid structure on interactions with TiO2 particles in ionic liquid assisted hydrothermal synthesis”, contract No.2014/15/D/ST5/02747. The authors also acknowledge Karina Kacperska for her support.
Zhong, J.; Li, J.; Zeng, J.; He, X.; Huang, S.; Jiang, W.; Li, M. Appl. Phys. A: Mater. Sci. Process.2014,115, 1231–1238. doi:10.1007/s00339-013-7965-z
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