Cheng Li,
Haifeng Zhang and
Chuanwei Cheng*
Shanghai Key Laboratory of Special Artificial Microstructure Materials and Technology, School of Physics Science and Engineering, Tongji University, Shanghai 200092, P. R. China. E-mail: cwcheng@tongji.edu.cn
First published on 30th March 2016
In this paper, we report a novel electrode of 3D ordered CdS/CdSe co-sensitized sea urchin-like SnO2/TiO2 nanotube arrays for photoelectrochemical hydrogen production. This novel photoanode presents excellent PEC performance, yielding a maximum photocurrent density of ∼6 mA cm−2 at 1.4 V vs. RHE under light illumination AM 1.5 (100 mW cm−2), which is due to the 3D structural effect of the SnO2/TiO2 sea urchin nanotubes, stepwise cascade band alignment between SnO2/TiO2 and CdS/CdSe as well as the improvement of light harvesting in the visible region.
Herein, we report an innovative electrode of 3D SnO2/TiO2 sea urchin-like nanotube arrays by combination of ZnO sea urchin structures as templates and atomic layer deposition of SnO2 and TiO2 for the first time. The hollow sea urchin nanotube structures might be more beneficial for quantum dots loading and electrolyte infiltration in contrast to that of nanowires structures. CdS and CdSe quantum dots are further used as co-sensitizer for extending the visible light absorption edge. PEC measurements demonstrate that CdS/CdSe co-sensitized 3D SnO2/TiO2 sea urchin-like nanotubes electrode presents the best performance in contrast to that of SnO2/TiO2 sea urchin-like nanotubes and only CdS sensitized one.
The 3D SnO2/TiO2 sea urchin like nanotubes arrays were fabricated by using the SnO2 hollow spheres/ZnO nanorods sea urchins as sacrificial templates and subsequent ALD deposition of SnO2 and TiO2 layer. The fabrication process is illustrated in Fig. S1† and the typical SEM images of SnO2/ZnO urchins are presented in Fig. S2.† It can be seen that the ZnO nanorods are radially grown on the surfaces of each microsphere, forming a periodical sea urchin pattern in a large area. After the ALD deposition of SnO2 and TiO2 and removal of ZnO templates, the SnO2/TiO2 nanotube sea urchin-like arrays were obtained. As shown in Fig. 1a, perfectly patterned sea urchin arrays are still reserved. From a high-magnification view in Fig. 1b, the overall diameter of individual SnO2/TiO2 nanotube sea urchin is about 5 μm. The SEM images of SnO2/TiO2 sea urchin-like nanotubes after CdS quantum dots sensitization and CdS/CdSe co-sensitization are displayed in Fig. 1c–f, respectively, it can be observed the quantum dots layer are uniformly coated on the nanotubes surfaces, without influencing the periodical characteristics. Besides, no obvious nanoparticles aggregation was observed. Further EDX measurement (Fig. S3†) confirms the chemical elements in CdS/CdSe sensitized SnO2/TiO2 sea urchin nanotube arrays.
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Fig. 1 SEM images of (a and b) 3D SnO2/TiO2 sea urchin-like nanotubes; CdS sensitized (c and d) and CdS/CdSe co-sensitized (e and f) 3D sea SnO2/TiO2 urchin-like nanotubes. |
The microstructures of the SnO2/TiO2 urchin-like nanotubes and quantum dots sensitized samples were further characterized by transmission electron microscopy (TEM) and HRTEM. The typical TEM image of SnO2/TiO2 nanotubes in Fig. 2a clearly demonstrates the core/shell hybrid nanotube morphology. From the TEM image (inset of Fig. 2a), it can be seen that the tube wall thickness of SnO2 and TiO2 are ∼10 nm and ∼5 nm, respectively. The HRTEM image of SnO2/TiO2 nanotube in Fig. 2b indicates that the SnO2 is crystalline. The measured lattice 0.24 nm is corresponding to the (200) plane of rutile phase of SnO2. The TEM and HRTEM image in Fig. 2c and d represent the structure of CdS sensitized SnO2/TiO2 urchin-like nanotubes, indicating that the CdS layer is distributed uniformly on the surface of the SnO2/TiO2 nanotube. As shown in Fig. 2d, a clear interface between CdS and TiO2 can be observed. The measured lattices 0.34 nm is corresponding to the (002) plane of CdS. The thickness of CdS layer is about 8 nm. Fig. 2e and f show the TEM and HR-TEM image of the of CdS/CdSe co-sensitized SnO2/TiO2 urchin-like nanotubes, suggesting that CdSe nanoparticles were deposited on the surface successfully. As shown in Fig. 2f, the measured lattice of 0.34 nm and 0.22 nm are corresponding to the (002) plane of CdS and the (110) plane of CdSe.
To further investigate the composition and chemical environment of the as-fabricated CdS/CdSe co-sensitized SnO2/TiO2 urchin-like nanotubes, X-ray photoelectron spectroscopy (XPS) was performed. The high-resolution XPS spectra in Fig. 3a shows the O peaks that were divided into three peaks with binding energy at 530.0, 530.4 and 533.3 eV, which may be ascribed to the Sn–O in SnO2,32 Ti–O in TiO2,33 and hydroxyl groups, respectively. The two peaks in Fig. 3b were corresponding to the Ti 2p3/2 and Ti 2p1/2 with binding energies of 458.8 and 464.7 eV.33 The spectra of Sn 3d in Fig. 3c shows two peaks of Sn 3d3/2 and Sn 3d5/2 with binding energies centered at 486.6 and 495.1 eV, respectively.32 As shown in Fig. 3d, the Cd 3d5/2 peak centered at 405.1 eV and the Cd 3d3/2 peak centered at 411.8 eV.33 The two peaks in Fig. 3e were corresponding to the S 2p3/2 and S 2p1/2 with binding energies of 160.1 and 161.5 eV, indicating that the valence state of S is −2.34 The two peaks centered at 53.9 and 54.8 eV in Fig. 3f are associated with the Se 3d5/2 and Se 3d3/2, which may be ascribed to the Cd–Se bonds.35
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Fig. 3 XPS spectra collected from CdS/CdSe co-sensitized 3D SnO2/TiO2 sea urchin-like nanotubes. (a) O 1s; (b) Ti 2p; (c) Sn 3d; (d) Cd 3d; (e) S 2p; (f) Se 3d. |
The optical characteristics of the as-fabricated CdS and CdS/CdSe sensitized SnO2/TiO2 sea urchin-like nanotubes were studied by collecting the diffuse light reflectance spectrum with UV-vis spectrophotometer. As shown in Fig. 4, the CdS/CdSe co-sensitized SnO2/TiO2 sea urchin-like nanotubes exhibits the best light harvesting ability in the whole measured wavelength scale in contrast to that of SnO2/TiO2 and CdS sensitized one. The absorption edge is extending to ∼650 nm, corresponding to the bandgap of CdSe quantum dots, which is improving the visible light harvesting ability greatly.
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Fig. 4 UV-vis diffuse reflectance spectrum of 3D SnO2/TiO2 urchin-like nanotubes, CdS sensitized and CdS/CdSe co-sensitized 3D SnO2/TiO2 urchin-like nanotubes. |
The PEC water splitting performance was evaluated by measuring the photocurrent density with a three-electrode electrochemical cell. Fig. 5a presents a group of the linear sweep voltammogram curves collected from SnO2/TiO2, CdS sensitized and CdS/CdSe co-sensitized SnO2/TiO2 sea urchin-like nanotubes photoanodes measured in the dark and under light illumination (AM 1.5, 100 mW−2). It can be seen that all the three samples present very small current density in the dark, while under light illumination, pronounced photocurrent density were observed, especially for the CdS and CdS/CdSe co-sensitized samples. It is worthy noting that the CdS/CdSe co-sensitized SnO2/TiO2 sea urchin-like nanotubes photoelectrode shows the best PEC performance, achieving a maximum photocurrent density of ∼6 mA cm−2 at 1.4 V vs. RHE, which is 15 times and 2 times larger than that of bare SnO2/TiO2 sea urchin-like nanotubes (0.4 mA cm−2) and CdS sensitized one (3 mA cm−2), respectively. The achieved photocurrent density value is also superior to most of the previous reported results in quantum dots sensitized photoelectrodes, such as CdS sensitized TiO2/ZnO urchins (∼3.6 mA cm−2),13 CdS sensitized TiO2 inverse opals (4.84 mA cm−2),4 ZnSe/CdS/CdSe triple-sensitized ZnO nanowire arrays (∼5.3 mA cm−2),36 and CdS/CdSe sensitized hollow TiO2 nanowire arrays (∼4 mA cm−2).37 This might be attributed to the 3D structural effect of SnO2/TiO2 sea urchin-like nanotubes that provides large surface area for quantum dots loading as well as the synergistic effect of CdS and CdSe quantum dots which improves the visible light absorption and charge transfer process. Fig. 5b presents the corresponding transient i–t curves of the three photoelectrodes collected under chopped light illumination (30 s every light/dark cycle) at the bias of 0.9 V vs. RHE, demonstrating excellent photoresponse ability and fast photoswitching property. What's more, the CdS/CdSe co-sensitized SnO2/TiO2 sea urchin-like nanotubes photoelectrode showed very excellent photo-stability with little decay under continuous light illumination, as shown in Fig. 5c.
To understand the charge transfer mechanism of CdS/CdSe sensitized SnO2/TiO2 sea urchin-like nanotubes, electrochemical impedance spectroscopy (EIS) measurement was conducted at open-circuit condition under simulated light illumination. Fig. 5d presents the Nyquist plots of the collected EIS data, which can be fitted by the physical model developed in similar quantum dots sensitized heterostructures.37,38 The semicircle in the high frequency (>104 Hz) in the Nyquist plots corresponds to the charge transfer in TiO2/FTO interface, while the second semicircle portion in the middle frequency range (1–103 Hz) corresponds to the charge transfer resistance at the photoelectrode/electrolyte interface. Apparently, the CdS/CdSe sensitized SnO2/TiO2 urchin-like nanotubes photoanode shows the smallest charge transfer resistance in contrast to that of SnO2/TiO2 and CdS sensitized one, which suggests that the stepwise cascade band alignment between CdS/CdSe and SnO2/TiO2 (as illustrated in Fig. 6b) are facilitating the photo-induced charge separation and transfer process.
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Fig. 6 (a) Scheme of the CdS/CdSe co-sensitized of SnO2/TiO2 sea urchin-like nanotube arrays. (b) Band alignment and charge transfer process between the CdS/CdSe and SnO2/TiO2. |
The scheme of urchin-like nanotubes arrays and processes of electron transfer in the CdS/CdSe co-sensitized SnO2/TiO2 urchin-like nanotubes photoelectrode can be simplified in Fig. 6a and b. As shown in Fig. 6b, under light illumination, the semiconductor SnO2/TiO2 and QDs absorb the photons and generated electron–hole pairs. Compared with SnO2 and TiO2, CdS has a higher conduction band edge, CdSe has a higher valence band edge, which is advantageous to the charge transportation.31 The stepwise cascade band alignment between the CdS/CdSe and SnO2/TiO2 is facilitating the photo-induced carrier separation and transfer process, as a result in reduction in the electron-holes recombination process. The higher electron mobility of SnO2 nanotubes would be beneficial for improving the charge collection efficiency.24
Based on the above discussions, the excellent PEC performance for 3D CdS/CdSe co-sensitized TiO2/SnO2 electrode can be explained as follows. First, the 3D urchin-like TiO2/SnO2 electrode provided increased surface area for both CdS and CdS quantum dots loading, leading to an enhancement of light harvesting, as evidenced in Fig. 4. Second, the stepwise cascade band alignment between the CdS/CdSe and SnO2/TiO2 is beneficial for the charge separation and transfer process, result in improving the charge separation and collection efficiency.
Footnote |
† Electronic supplementary information (ESI) available: Scheme of the fabrication process of CdS/CdSe sensitized SnO2/TiO2 urchin nanotubes arrays, SEM image of ZnO sea urchin structure and EDX spectrum of CdS/CdSe co-sensitized SnO2/TiO2 sea urchin-like nanotube arrays. See DOI: 10.1039/c6ra02176j |
This journal is © The Royal Society of Chemistry 2016 |