- Nano Express
- Open Access
Electrochemically hydrogenated TiO2 nanotubes with improved photoelectrochemical water splitting performance
© Xu et al.; licensee Springer. 2013
- Received: 25 July 2013
- Accepted: 13 September 2013
- Published: 18 September 2013
One-dimensional anodic titanium oxide (ATO) nanotube arrays hold great potential as photoanode for photoelectrochemical (PEC) water splitting. In this work, we report a facile and eco-friendly electrochemical hydrogenation method to modify the electronic and PEC properties of ATO nanotube films. The hydrogenated ATO (ATO-H) electrodes present a significantly improved photocurrent of 0.65 mA/cm2 in comparison with that of pristine ATO nanotubes (0.29 mA/cm2) recorded under air mass 1.5 global illumination. The incident photon-to-current efficiency measurement suggests that the enhanced photocurrent of ATO-H nanotubes is mainly ascribed to the improved photoactivity in the UV region. We propose that the electrochemical hydrogenation induced surface oxygen vacancies contribute to the substantially enhanced electrical conductivity and photoactivity.
- TiO2 nanotubes
- Electrochemical reductive doping
- Photoelectrochemical water splitting
Continued research efforts over the past few decades on solar water splitting have led to a substantial improvement in both scientific understanding and technical application[1–4]. Because of its abundance, nontoxicity, and stability, TiO2 is one of the most promising photoanodes in the solar water splitting system. So far the solar-to-hydrogen (STH) efficiency of TiO2-based photoanodes is limited by a wide bandgap (3.0 to 3.2 eV) and numerous electron–hole recombination centers. A variety of approaches have been explored to enhance the visible light activity of TiO2, such as metal doping or nonmetal doping[7, 8].
Recently, hydrogenation of TiO2, with intentionally introduced Ti3+ or oxygen vacancy states, has been proved to be an effective strategy for improving the electronic conductivity and photoresponse property[9–14]. Annealing processes in hydrogen atmosphere either under high temperature[13, 14] or by a long processing duration are two most employed ways. However, the need for either high-energy consumption or expensive facility would limit its practical application. Alternatively, the electrochemical reductive doping process provides another simpler approach for TiO2 hydrogenation. Under an external electric field, hydrogen is driven into the TiO2 lattice and reduces Ti4+ to Ti3+[15, 16]. The intentionally introduced donor states associated with enhanced conductivity have delivered a variety of applications in template synthesis[17, 18], electrochemical supercapacitors, and photovoltaic devices.
Moreover, in comparison with conventional nanoparticles, one-dimensional anodic titanium oxide (ATO) nanotube arrays with well-defined tubular structures provide a direct pathway for charge transport[21–23], thus possessing promising capabilities in photoelectrochemical (PEC) system. Herein, the electrochemical reductive doping approach is conducted on ATO nanotubes with the aim of improving the photoelectrochemical activity of TiO2 for hydrogen production through water splitting. The hydrogenated ATO nanotubes (ATO-H) showed significantly increased UV light response compared with the pristine ATO electrode. The hydrogen-induced oxygen vacancies in ATO-H are responsible for the improved conductivity and photoresponse.
Ti foils (99.7%, 0.2 mm thickness, Shanghai Shangmu Technology Co. Ltd) were ultrasonically cleaned in acetone, ethanol, and deionized water successively after an annealing process (450°C for 2 h). Then electrochemical polish was carried out in a solution of acetic acid and perchloric acid which determined the flat surface of the Ti foils. ATO nanotube films were made by two-step anodization in ethylene glycol electrolyte containing 0.3 wt.% NH4F and 10 vol.% H2O. First-step anodization was performed at 150 V for 1 h in a conventional two-electrode configuration with a carbon rod as cathode electrode. The as-anodized nanotube films were removed from the Ti foil with adhesive tape. Second-step anodization was performed under the same condition for 1 h. The ATO products were crystallized in ambient air at 150°C for 3 h, then up to 450°C for 5 h with a heating rate of 1°C/min.
The electrochemical reductive doping process was performed in a two-electrode system at room temperature, employing the ATO nanotubes and a Pt electrode as the cathode and anode, respectively, with the distance between the two electrodes exactly fixed at 2.5 cm. The crystallized ATO nanotubes were immersed in 0.5 M Na2SO4 aqueous solution, and a voltage of 5 V was imposed between the electrodes. The reductive doping duration was maintained in the range of 5 to 40 s, and the optimum time was found to be 10 s. Finally, the ATO nanotubes were taken out, washed with deionized water, and dried for measurements.
The morphology and crystalline structure of nanotube films were characterized using field-emission scanning electron microscope (FESEM, FEI Quanta 600, FEI Company, Hillsboro, OR, USA), transmission electron microscope (HRTEM, JEM-2100F, JEOL Ltd., Akishima, Tokyo, Japan), and X-ray diffractometer (XRD, D8 Discover diffractometer, Bruker AXS GMBH, Karlsruhe, Germany). Raman spectroscopy (DXR Raman microscope with 532-nm excitation laser, Thermo Fisher Scientific, Waltham, MA, USA) was employed for chemical state analysis. Time-resolved photoluminescence (TRPL) spectra were recorded at ambient temperature with a time-correlated single-photon counting (TCSPC) spectrometer (Photon Technology International, Inc., Birmingham, NJ, USA), where a pulsed laser at 375 nm with an average power of 1 mW (100 fs, 80 MHz) was used as the excitation source.
The PEC water splitting performances of the ATO nanotubes without and with electrochemical hydrogenation were evaluated by AUTOLAB using a three-electrode configuration with the nanotube films (1 × 1 cm2) as working electrode, Ag/AgCl (3 M KCl) electrode as reference electrode, and a platinum foil as counter electrode. The supporting electrolyte was 1 M potassium hydroxide (KOH, pH = 14) containing 1 wt.% of ethylene glycol solution, where ethylene glycol acted as a potential hole scavenger (electron donor) to minimize the recombination of charge carriers. The photocurrent was measured at a potential of 0 V (vs Ag/AgCl) under chopped light irradiation with UV light (5.8 mW/cm2 at 365 nm) and simulated solar illumination (100 mW/cm2) from a Xe lamp coupled with an air mass 1.5 global (AM 1.5G) filter (Newport no. 94063A). The incident photon-to-current conversion efficiency (IPCE, DC mode) was measured in three-electrode configuration by an AUTOLAB electrochemical station with the assistance of a commercial spectral response system (QEX10, PV Measurements, Inc., Boulder, CO, USA). In order to record the stable photoresponse from photoanodes, each wavelength was held for 3 min before the photocurrent measurements. Impedance measurements were performed under dark condition at open-circuit potential over a frequency range of 100 kHz to 0.1 Hz with an amplitude of 10 mV.
Figure 1d displays the Raman spectra of ATO nanotubes treated with different reductive processing times (denoted as ATO-H-5, ATO-H-10, and ATO-H-30 for 5-, 10-, and 30-s treatments, respectively). The six Raman vibrational mode of anatase TiO2 samples can be found at 148.4 cm-1 (Eg(1)), 200.5 cm-1 (Eg(2)), 399.1 cm-1 (B1g(1)), 641.2 cm-1 (Eg(3)), 520.6 cm-1 (A1g), and 519 cm-1 (B1g(2) superimposed with 520.6 cm-1), which is in agreement with the above XRD results. A slight blueshift and broadening of Eg(1) and Eg(2) peaks are observed in the ATO-H-10 sample, suggesting increased surface disorder due to the introduced oxygen vacancies. According to the above analysis, the possibly introduced defect states originate from the formation of oxygen vacancies on ATO nanotubes.
Figure 2b, and c show the photocurrent of ATO and ATO-H-10 under illuminations of chopped UV (5.8 mW/cm2 at 365 nm) and simulated solar light (100 mW/cm2) at a constant potential of 0 V (vs Ag/AgCl). In comparison with the photocurrent density generated on pristine ATO (0.25 mA/cm2 under UV irradiation and 0.29 mA/cm2 under solar irradiation), the ATO-H-10 electrode delivers a much improved performance (0.56 mA under UV irradiation and 0.65 mA/cm2 under solar irradiation). Meanwhile, Figure 2d presents the chronoamperometric curves under simulated solar illumination for characterizing the long-term stability of nanotube photoelectrodes. Both curves were kept stable within the measurement period, indicating good stability after electrochemical hydrogenation.
Linear sweeps voltammetry (LSV) is a voltammetric method where the potential between the working electrode and a reference electrode is linearly swept in time with simultaneously recorded current. In the PEC water-splitting system, LSV is widely employed to characterize the photoelectrodes’ performance with quantitative open circuit voltage (Voc), short-circuit current (Jsc), fill factor (FF), and light-to-hydrogen efficiency. However, unlike most solid-state solar cells, the linear sweeps in this liquid system are strongly dependent on the scan rate. Under a fast potential scan, the thickness of diffusion layer will decrease from the electrode in comparison with the one under a slow scan. Consequently, the ionic flux towards electrode surface associated with current density will be increased. Therefore, the scan rate is worthy of serious consideration in evaluating the electrode performance. One could give an overestimated and misleading STH efficiency if an inappropriate high scan rate was applied.
where V is the applied bias voltage vs reversible hydrogen electrode (RHE), I is the photocurrent density at the measured bias, and Jlight is the irradiance intensity of 100 mW/cm2. The pristine ATO exhibits a STH efficiency of 0.19% at -0.64 V (vs Ag/AgCl), while the ATO-H electrode yields a much improved efficiency (η = 0.30%) at -0.48 V (vs Ag/AgCl). Moreover, the quartz window reflects more than 4% of the solar irradiance, which means that the internal STH efficiencies are higher than the calculated values. Using front-side illumination configuration could reduce this loss and further boost the conversion efficiency.
IPCE measurements are carried out to investigate the contribution of each monochromatic light to the photocurrent density. Compared with the measurements based on the wide band light source without taking into account the differences between the spectra of the light source and the solar spectrum, and/or reliable calibration, which may vary from different research laboratories, the intensity-independent IPCE provides a reliable method to characterize the wavelength dependent photoresponse. The IPCE is calculated as a function of wavelength using IPCE = (1,240 (mW⋅nm/mA)I) / (λJlight), where λ is the incident light wavelength (nm) and I and Jlight are the photocurrent density (mA/cm2) and incident light irradiance (mW/cm2) at a specific wavelength.
Figure 3c shows the IPCE plots of ATO and ATO-H-10 at zero bias vs Ag/AgCl. The results indicate that the enhanced photocurrent is mainly contributed by UV response due to electrical conductivity modification. Reductive doping gives rise to a pronounced enhancement in full UV region (300 to 400 nm) with a maximum value of 82% at 360 nm. The decrease at shorter wavelengths could be attributed to the unwanted light reflection or absorption before arriving to a photoanode. In the longer wavelength region, IPCE plots represent abrupt decreases from approximately 49% (ATO) and approximately 74% (ATO-H-10) at 370 nm to less than 2% at 410 nm, which is determined by the recombination of charge carriers in the wide bandgap (approximately 3.2 eV) anatase TiO2. A weak photoactivity of pristine ATO nanotube in 400 to 600 nm could be ascribed to fluorine doping during anodization in NH4F-containing electrolytes[9, 31]. In addition, a slightly enhanced photocurrent can also be observed in the visible range (410 to 600 nm) on ATO-H-10 electrode (inset of Figure 3c). The oxygen vacancy states are generally localized with energies of 0.75 to 1.18 eV below the conduction band, which is lower than the redox potential for hydrogen evolution[32, 33], while a high vacancy concentration could produce shallow donor levels just below the conduction band, which in turn provides enough energy for water splitting. The experimental results suggest the formation of shallow levels which is responsible for the slightly enhanced visible light activity.
It is known that PEC performance of the electrode is determined by charge separation and transfer process. Besides offering increased donor states, the introduced defect states would also serve as recombination centers for electron–hole pairs and consequently inhibit the charge collection. The visible luminescence band of anatase TiO2 is caused by donor-acceptor recombination, which is closely related to both trapped electrons and trapped holes. In the nanocrystalline electrode, photoexcited carriers are readily captured in the inherent trap states. Trapping and thermally detrapping mechanisms will determine the slow decay process. It is believed that the inherent shallow trap states in pristine ATO, serving as electron trapping sites, mainly contribute to the slow decay process. Subsequently, electrochemical hydrogenation could introduce more defect states into shallow energy levels to capture excited electrons, which will prolong the relaxation processes with the corresponding longer lifetime. The dynamic characteristics of photogenerated carriers are revealed by room-temperature TRPL spectroscopy. Figure 4b displays the TRPL curves of the different electrodes recorded at 413 nm with a 375-nm pulsed laser as excitation source. The ATO-H-10 electrode shows a somewhat longer lifetime compared with the pristine ATO electrode. This means that the electrochemical reductive process is an efficient strategy to improve electrode conductivity, with a slightly increased recombination rates. By utilizing single exponential decay fitting on the obtained curves, the averaged photoluminescence lifetimes of ATO and ATO-H-10 are calculated to be 537 and 618 ps, respectively.
In conclusion, the electrochemical reductive doping processes are carried out to produce hydrogenated ATO photoanodes to improve PEC water splitting efficiency. A -5-V bias voltage, with only 10 s of processing time, yields a substantially enhanced photocurrent density of 0.29 to 0.65 mA/cm2. IPCE results indicate that the enhanced STH efficiency in ATO-H-10 is dominantly contributed by the improved photoactivities in the UV region. The electrochemically induced oxygen vacancies lead to increased donor density, which is responsible for the enhanced photocurrent with slightly increased parasitic recombination. This eco-friendly approach opens up a novel strategy for significantly improving the photoanode performance and provides potential for large-scale productions.
XYC, XFZ, and DDL designed the experiments. CX, XHF, and LFL carried out the experiments. CX, YS, CWC, and DFL performed electrode characterization and data analysis. CX and DDL wrote the paper. All authors read and approved the final manuscript.
We thank Professor Xiangyang Kong for his helpful discussions and technical assistance. This work is financially supported by the National Natural Science Foundation of China (grant nos. 61171043, 51077072, 11174308 and 51102271), Shell Global Solutions International B.V. (PT31045), the Natural Science Foundation of Shanghai (11ZR1436300), and the Shanghai Municipal Human Resources and Social Security Bureau (2011033).
- Fujishima A, Honda K: Electrochemical photolysis of water at a semiconductor electrode. Nature 1972, 238: 37–38.View ArticleGoogle Scholar
- Hwang YJ, Hahn C, Liu B, Yang PD: Photoelectrochemical properties of TiO2 nanowire arrays: a study of the dependence on length and atomic layer deposition coating. Acs Nano 2012, 6: 5060–5069.View ArticleGoogle Scholar
- Li ZS, Luo WJ, Zhang ML, Feng JY, Zou ZG: Photoelectrochemical cells for solar hydrogen production: current state of promising photoelectrodes, methods to improve their properties, and outlook. Energ Environ Sci 2013, 6: 347–370.View ArticleGoogle Scholar
- Pinaud Blaise A, Benck Jesse D, Seitz Linsey C: Technical and economic feasibility of centralized facilities for solar hydrogen production via photocatalysis and photoelectrochemistry. Energy Environ Sci 2013, 6: 1983–2002.View ArticleGoogle Scholar
- Chen X, Mao SS: Titanium dioxide nanomaterials: synthesis, properties, modifications, and applications. Chem Rev 2007, 107: 2891–2959.View ArticleGoogle Scholar
- Zhao W, Chen CC, Li XZ, Zhao JC, Hidaka H, Serpone N: Photodegradation of sulforhodamine-B dye in platinized titania dispersions under visible light irradiation: Influence of platinum as a functional co-catalyst. J Phys Chem B 2002, 106: 5022–5028.View ArticleGoogle Scholar
- Lai CW, Sreekantan S: Study of WO3 incorporated C-TiO2 nanotubes for efficient visible light driven water splitting performance. J Alloy Compd 2013, 547: 43–50.View ArticleGoogle Scholar
- Batzill M, Morales EH, Diebold U: Influence of nitrogen doping on the defect formation and surface properties of TiO2 rutile and anatase. Phys Rev Lett 2006, 96: 026103.View ArticleGoogle Scholar
- Wang GM, Wang HY, Ling YC, Tang YC, Yang XY, Fitzmorris RC, Wang CC, Zhang JZ, Li Y: Hydrogen-treated TiO2 nanowire arrays for photoelectrochemical water splitting. Nano Lett 2011, 11: 3026–3033.View ArticleGoogle Scholar
- Naldoni A, Allieta M, Santangelo S, Marelli M, Fabbri F, Cappelli S, Bianchi CL, Psaro R, Dal Santo V: Effect of nature and location of defects on bandgap narrowing in black TiO2 nanoparticles. J Am Chem Soc 2012, 134: 7600–7603.View ArticleGoogle Scholar
- Chen XB, Liu L, Yu PY, Mao SS: Increasing solar absorption for photocatalysis with black hydrogenated titanium dioxide nanocrystals. Science 2011, 331: 746–750.View ArticleGoogle Scholar
- Zheng ZK, Huang BB, Lu JB, Wang ZY, Qin XY, Zhang XY, Dai Y, Whangbo MH: Hydrogenated titania: synergy of surface modification and morphology improvement for enhanced photocatalytic activity. Chem Commun 2012, 48: 5733–5735.View ArticleGoogle Scholar
- Lu XH, Wang GM, Zhai T, Yu MH, Gan JY, Tong YX, Li Y: Hydrogenated TiO2 nanotube arrays for supercapacitors. Nano Lett 2012, 12: 1690–1696.View ArticleGoogle Scholar
- Jiang XD, Zhang YP, Jiang J, Rong YS, Wang YC, Wu YC, Pan CX: Characterization of oxygen vacancy associates within hydrogenated TiO2: a positron annihilation study. J Phys Chem C 2012, 116: 22619–22624.View ArticleGoogle Scholar
- Chen WP, Wang Y, Dai JY, Lu SG, Wang XX, Lee PF, Chan HLW, Choy CL: Spontaneous recovery of hydrogen-degraded TiO2 ceramic capacitors. Appl Phys Lett 2004, 84: 103–105.View ArticleGoogle Scholar
- Chen WP, Wang Y, Chan HLW: Hydrogen: a metastable donor in TiO2 single crystals. Appl Phys Lett 2008, 92: 112907–112910.View ArticleGoogle Scholar
- Li DD, Chien CJ, Deora S, Chang PC, Moulin E, Lu JG: Prototype of a scalable core-shell Cu2O/TiO2 solar cell. Chem Phys Lett 2011, 501: 446–450.View ArticleGoogle Scholar
- Macak JM, Gong BG, Hueppe M, Schmuki P: Filling of TiO2 nanotubes by self-doping and electrodeposition. Adv Mater 2007, 19: 3027–3031.View ArticleGoogle Scholar
- Zhou H, Zhang YR: Enhancing the capacitance of TiO2 nanotube arrays by a facile cathodic reduction process. J Power Sources 2013, 239: 128–131.View ArticleGoogle Scholar
- Li DD, Chang PC, Chien CJ, Lu JG: Applications of tunable TiO2 nanotubes as nanotemplate and photovoltaic device. Chem Mater 2010, 22: 5707–5711.View ArticleGoogle Scholar
- Shankar K, Basham JI, Allam NK, Varghese OK, Mor GK, Feng XJ, Paulose M, Seabold JA, Choi KS, Grimes CA: Recent advances in the use of TiO2 nanotube and nanowire arrays for oxidative photoelectrochemistry. J Phys Chem C 2009, 113: 6327–6359.View ArticleGoogle Scholar
- Varghese OK, Paulose M, LaTempa TJ, Grimes CA: High-rate solar photocatalytic conversion of CO2 and water vapor to hydrocarbon fuels. Nano Lett 2009, 9: 731–737.View ArticleGoogle Scholar
- Li H, Cheng JW, Shu SW, Zhang J, Zheng LX, Tsang CK, Cheng H, Liang FX, Lee ST, Li YY: Selective removal of the outer shells of anodic TiO2 nanotubes. Small 2013, 9: 37–44.View ArticleGoogle Scholar
- Liu ZY, Zhang QQ, Zhao TY, Zhai J, Jiang L: 3-D vertical arrays of TiO2 nanotubes on Ti meshes: efficient photoanodes for water photoelectrolysis. J Mater Chem 2011, 21: 10354–10358.View ArticleGoogle Scholar
- Xue XX, Ji W, Mao Z, Mao HJ, Wang Y, Wang X, Ruan WD, Zhao B, Lombardi JR: Raman investigation of nanosized TiO2: effect of crystallite size and quantum confinement. J Phys Chem C 2012, 116: 8792–8797.View ArticleGoogle Scholar
- Ohsaka T, Izumi F, Fujiki Y: Raman-spectrum of anatase, TiO2. J Raman Spectrosc 1978, 7: 321–324.View ArticleGoogle Scholar
- Prasad MA, Sangaranarayanan MV: Analysis of the diffusion layer thickness, equivalent circuit and conductance behaviour for reversible electron transfer processes in linear sweep voltammetry. Electrochim Acta 2004, 49: 445–453.View ArticleGoogle Scholar
- Zhang ZH, Zhang LB, Hedhili MN, Zhang HN, Wang P: Plasmonic gold nanocrystals coupled with photonic crystal seamlessly on TiO2 nanotube photoelectrodes for efficient visible light photoelectrochemical water splitting. Nano Lett 2013, 13: 14–20.View ArticleGoogle Scholar
- Murphy AB, Barnes PRF, Randeniya LK, Plumb IC, Grey IE, Horne MD, Glasscock JA: Efficiency of solar water splitting using semiconductor electrodes. Int J Hydrogen Energ 2006, 31: 1999–2017.View ArticleGoogle Scholar
- Welte A, Waldauf C, Brabec C, Wellmann PJ: Application of optical absorbance for the investigation of electronic and structural properties of sol–gel processed TiO2 films. Thin Solid Films 2008, 516: 7256–7259.View ArticleGoogle Scholar
- Park H, Choi W: Effects of TiO2 surface fluorination on photocatalytic reactions and photoelectrochemical behaviors. J Phys Chem B 2004, 108: 4086–4093.View ArticleGoogle Scholar
- Zuo F, Wang L, Wu T, Zhang ZY, Borchardt D, Feng PY: Self-doped Ti3+ enhanced photocatalyst for hydrogen production under visible light. J Am Chem Soc 2010, 132: 11856–11857.View ArticleGoogle Scholar
- Cronemeyer DC: Infrared absorption of reduced rutile TiO2 single crystals. Phys Rev 1959, 113: 1222–1226.View ArticleGoogle Scholar
- Justicia I, Ordejon P, Canto G, Mozos JL, Fraxedas J, Battiston GA, Gerbasi R, Figueras A: Designed self-doped titanium oxide thin films for efficient visible-light photocatalysis. Adv Mater 2002, 14: 1399–1402.View ArticleGoogle Scholar
- Ye MD, Gong JJ, Lai YK, Lin CJ, Lin ZQ: High-efficiency photoelectrocatalytic hydrogen generation enabled by palladium quantum dots-sensitized TiO2 nanotube arrays. J Am Chem Soc 2012, 134: 15720–15723.View ArticleGoogle Scholar
- Wang XL, Feng ZC, Shi JY, Jia GQ, Shen SA, Zhou J, Li C: Trap states and carrier dynamics of TiO2 studied by photoluminescence spectroscopy under weak excitation condition. Phys Chem Chem Phys 2010, 12: 7083–7090.View ArticleGoogle Scholar
- Wakabayashi K, Yamaguchi Y, Sekiya T, Kurita S: Time-resolved luminescence spectra in colorless anatase TiO2 single crystal. J Lumin 2005, 112: 50–53.View ArticleGoogle Scholar
This article is published under license to BioMed Central Ltd. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.