The brookite nanosquares were synthesized by a novel mild one-step hydrothermal process as illustrated in Scheme 1. Titanium cations of water-soluble titanium compounds usually exist as 6-fold-coordinated, charged complexes [TiL6]z± in an aqueous medium. The nature of the ligand L is in connection with the pH value and the species that can coordinate with Ti4+ in the solution. In our case, two kinds of water-soluble titanium precursors were used simultaneously in the synthesis process. As suggested by the literature, the experiment involved two complexes: one is [Ti(OH)2Cl2(OH2) 2]0 octahedron formed [26] when TiOCl2 was added into HCl water solution; the other spicies are [Ti(C3H4O3)2(OH)2]2− octahedrons generated via dissociation of titanium-contained complex TiBALDH[27]. The formations of these octahedron complexes have been formed by the reaction equations (1) and (2) as follows:
TiOCl2 + 3H2O → [Ti(OH) 2Cl2(OH2) 2] 0 (1)
(NH4)2[Ti(C3H4O3)2(OH)2] → 2 NH4+ + [Ti(C3H4O3)2(OH)2]2− (2)
Under hydrothermal conditions and a strong acid environment, along with the condensation reactions, these two kinds of octahedron complexes can form dimers, trimers, small chains of octahedra, and then layered titanate of brookite. Tomita et al. [28] have found that metastable phases often crystallize first in chimie douce methods at low temperatures because their nucleolus only needs lower supersaturation. Once the nucleation of the brookite phase had occurred, the growth of the crystallites would continue because of the lower activation energy than the nucleation of another new phase. As a result, with the proceeding of further condensation, solid oxide appeared through the formation and growth of the nuclei and finally crystallized to brookite TiO2. Previous theoretical calculations revealed that the {210} surface energy of brookite TiO2 is 0.70 J/m2, which makes this surface one of the most stable surfaces[29]. In our case, the exposed surface of the obtained brookite nanosquare is also {210} (seen in Fig. 2e).
Figure 1a depicts the XRD patterns of the as-prepared powder. It is found that all diffraction peaks of the product in XRD can be indexed to the diffraction peaks of orthorhombic brookite (JCPDS 65-2448). And there are no reflections assignable to anatase or rutile TiO2 phases which guarantees the high purity of the obtained powder. Therefore, the synthesized samples are concluded to be pure brookite phase. The mean crystallite size was determined to be 50.7 nm from the diffraction patterns using the Scherrer equation.
On the basis of the theory of space group, brookite lattice possesses lower symmetry (D2h) and larger unit cells which lead to a large amount of Raman active phonons. Raman spectroscopy is considered a very effective way to identify the existence of brookite in a sample because brookite reveals a characteristic complicated vibrational spectrum compared to the other TiO2 polymorphs. Figure 1b shows the Raman spectra of the prepared TiO2 sample. The Raman spectrum of the brookite TiO2 usually shows 15 vibration bands in the range of 100 ~ 700 cm− 1. These bands can be assigned to the modes of A1g (155, 194, 247, 412, 636cm − 1), B1g (213, 322, 501 cm− 1), B2g (366, 395, 460, 583 cm− 1), and B3g (172, 287, 545 cm− 1), respectively[30, 31]. In our case, the spectra shows the characteristic bands of brookite include the most intense A1g mode (155 cm− 1) and other 12 weaker peaks at 126, 194, 213, 248, 287, 322, 365, 412, 461, 500, 545, 583, and 636 cm− 1 assigned as A1g, B1g, B2g, and B3g vibrations, respectively. And there are no apparent vibration bands related to the anatase and rutile in the spectrum. XPS experiments were applied to analyze the chemical binding states of brookite. The Ti 2p XPS spectra of is presented in Fig. 1(c). Ti 2p 1/2 and Ti 2p 3/2 peaks locate at the binding energies of 458.5 and 464.3 eV, respectively, and the datas are correspond to the lattice chemical bonding of TiO2 as the earlier reports[12, 16]. XRD, XPS and Raman studies confirm that the obtained product is pure brookite phases.
To obtain the morphological features of the as-prepared TiO2 powders, the sample was characterized by using TEM, SAED, and HRTEM, and the results are displayed in Fig. 2. Figure 2a and 2b show that the major morphological feature of the sample is a regular square shape in the almost same size with smooth edges. To examine the uniformity of the synthesized brookite TiO2 nanosquares, the mean edge length of nanosquares is statistically analyzed. The results show that the average value of the square edge length is ∼51 nm with a narrow size distribution from 30 to 70 nm(Fig. 2c). It is consistent with results from the the crystallite size calculated by using the Scherrer equation.
The HRTEM image (Fig. 2d, 2e) reveals that the lattice spacing is 0.351 nm, which is coherent with the early reported value of brookite (210) planes[29, 30]. The clear lattice fringes indicate the high crystallinity of the prepared brookite nanosquares. The SAED pattern is shown in Fig. 2f which represent the diffraction rings with light point indexed to (210), (211), (221), (321), and (400) planes of TiO2 brookite structure. This result proves that the prepared TiO2 is brookite nanosquares and which is consistent with XRD and Ramman results.
Figure 3a depicts the UV-vis diffuse reflectance absorption spectra (DRS) of the obtained brookite TiO2 nanosquares. The absorption band (band edges at 377.6 nm) at 290 nm is attributed to the intrinsic bandgap absorption of crystalline brookite TiO2. The bandgap energy (Eg) for the indirect transition of the brookite TiO2 nanosquares can be estimated through a Tauc plot[32, 33] (inset in Fig. 3a), which is 3.28 eV. The bandgap energy of the brookite TiO2 nanosquares was consistent with the previous investigation [34, 35].
The photocatalytic activity of the as prepared brookite TiO2 nanossquares was evaluated under UV irradiation using Rhodamine B as a probe molecule and the degradation curve was shown in Fig. 3b. When blank experiments were carried out, the self-photolysis of RhB was negligible in degradation time. About 70% of RhB is degraded by P25 within the prescribed time. Comparatively, brookite nanosquares showed excellent photo-catalytic properties in the decolorization of RhB with 96% in 180 min. The results indicate that the synthesized brookite nanosquares exhibit better activity on RhB degradation than Degussa P25. The better photocatalytic property of the prepared brookite TiO2 nanosquares could be attributed to the higher bandgap, and conduction band potential[36, 37], improved charge transport properties and effective charge separation[38–39], which prevents recombination of photogenerated electron-hole pairs.