WO3 and W2N nanowire arrays for photoelectrochemical hydrogen production

https://doi.org/10.1016/j.ijhydene.2009.09.031Get rights and content

Abstract

Tungsten oxide (WO3) nanowire array samples were nitrided in a NH3 atmosphere to get complete conversion to tungsten nitride (W2N) nanowires. UV–vis absorption spectroscopy shows that the band gap of WO3 reduced from 2.9 eV to 2.2 eV after nitridation to W2N. Photoelectrochemical properties of both WO3 and W2N nanowire array electrodes were investigated. WO3 nanowire arrays show maximum incident photon-to-current conversion efficiency of 85% at 370 nm at 1.2 V vs. SCE. The high quantum efficiency is attributed to the nanowire architecture which ensures efficient light absorption and charge transport. The nanowire arrays were stable even up to 8 h of continuous gas evolution. W2N nanowire arrays showed good photoactivity even at moderate bias. However, the pure W2N electrodes were unstable with respect to photocorrosion. The mixed phase W2N–WO3 nanowires showed improvement in stability compared to pure W2N nanowire arrays.

Introduction

Solar photolysis of water is one of the cleanest ways of producing hydrogen. The three main thermodynamic requirements of a semiconductor for spontaneous photolysis are (a) its band gap must be higher than 1.23 eV (b) its band edge positions must straddle the hydrogen and oxygen redox potential, and c) they must be stable against photocorrosion. See review by Bak et al. (2002) [1] for more extensive discussion. Although many metal phosphides and chalcogenides, such as GaP and CdS, have narrow band gaps that are suitable for water splitting, they are unstable against photo-anodic dissolution. Most of the currently used semiconductors that are stable are metal oxides such as TiO2 and WO3, but have wide band gaps (>3 eV), and thus only absorb ultraviolet photons. Band gap reduction of metal oxides (MO) with the addition of elements (Y) such C, N and S to form solid solutions (MO1−xYx) for enhanced visible light absorption have been reported previously for TiO2, WO3, In2O3 and ZnO [2], [3], [4], [5]. In TiO2 alloys, the atomic orbital (typically 2p or 3p) of foreign elements are known to mix with the O 2p orbital to create states within the band gap that give rise to visible light activity. However in such materials, inability to incorporate high concentration of dopant and degradation of crystallinity [6] with incorporation has been reported. It has been theoretically [7] and experimentally [8] shown that the nitride counterparts of metal oxide have lower band gap than the corresponding oxides. For example, the band gap of Ta2O5, decreased from 4.0 eV to 2.1 eV after conversion to metal nitrides, Ta3N5 [8]. Many transition metal nitrides are thought to be stable against corrosion similar to their oxide counterparts, but not have been tested so far. Herein, we report the investigation of tungsten nitride, W2N, as a potential candidate for a stable photocatalyst for water decomposition utilizing solar light.

In the recent years, transition metal nitrides such as W2N have gained considerable interest for other applications because of their unique properties such as high melting point (>2000 K), exceptional hardness (>10 Gpa), chemical inertness in acidic and basic solutions, durability, good electrical conductivity and radiation resistance. They have long been known to be an effective heterogeneous catalysts for a number of reactions such as hydrodesulphurization [9], and NO dissociation [10]. It has been reported that in many of these reactions metal nitride has catalytic activities resembling that of noble metals such as platinum. Recent study by Zhonga et al. (2007) [11] showed that the W2N is a good electrocatalyst for oxygen reduction reaction. They have also been used as a barrier coating in copper interconnects. Although metal nitrides such as WNx finds many industrial application there is still a lack of even fundamental electronic and optical properties such as band gap. In this paper, we have studied the structural, optical and photoelectrochemical properties of W2N and WO3 nanowire arrays. This is so far the first report of W2N as a material for photocatalyst.

Apart from the thermodynamic requirements, a suitable photoelectrode must also exhibit the following characteristics: (a). efficient charge transport through the semiconductor; (b). low overpotentials for the redox reactions; (c). low cost; and (d). high light harvesting efficiency. Nanoparticle electrodes have very high interfacial contact area which can make up for the slow kinetics of water oxidation reaction. However, numerous studies have shown that electron transport in these networks occurs by random hoping between particles. In fact, poor charge transport through nanocrystalline material is the one of the main factors in limiting the photocurrent of many semiconductors. Such poor transport combined with the inherently slow water oxidation reactions often results in the high degree of electron recombination either with the defect or trap states or within grain boundaries. To overcome this problem and to maximize both light harvesting and charge collection efficiency, one may use single crystalline 1-D nanowire array electrodes which offer several advantages. Since charge carriers are required to move axially along the length of the nanowire, they provide direct and faster electron transport to the back contact. This is shown schematically in Fig. 1. Array architectures provide longer dimension for light absorption [12]. Recombination at the grain boundary is avoided due to the single crystal nature of the wire. There have been several reports on the use of nanowires in other application such as dye sensitized solar cells [13], [14], [15]. However, there have been very few reports for water splitting reactions [16], [17]. For all the above reasons, we investigated the photoelectrochemical performance of WO3 and W2N nanowire array electrodes.

Section snippets

Experiments

Tungsten oxide nanowire arrays were synthesized in a specially designed hot wire chemical vapor deposition reactor setup. The detailed description of the reactor setup and the growth mechanism is described elsewhere [18]. Briefly, the technique involves flow of oxygen over a hot metal filament to create the respective metal oxide vapors which then diffuse and deposit over the cooler region of the reactor walls or substrate. The substrates were ultrasonically cleaned in ethanol and dried under

Morphology and crystallinity

Fig. 2A and B shows the SEM images of WO3 nanowire array grown on FTO and tungsten substrates respectively. Oxidation of W18O49 nanowire deposit in ambient air resulted in a color change from blue to greenish yellow and the corresponding XRD spectrum (not shown) indicated a change from monoclinic to orthorhombic phase. The color of the WO3 sample after nitridation changed to brownish black. SEM images showed that WO3 array film grown on quartz or FTO substrates typically consists of a thin

Conclusions

WO3 nanowire array samples showed good photocurrents (∼1.6 mA/cm2) under AM 1.5 solar light. WO3 nanowire array shows an IPCE of ∼85%, which is highest seen for WO3 electrodes. Prolonged photolysis up to 8 h shows very little degradation. In order to further improve the photoactivity, WO3 were nitrided to form W2N which had a smaller band gap as measured by UV–vis and photoluminescence measurements. W2N showed n-type behavior and good photoactivity even at moderate bias. The electrode underwent

Acknowledgments

The authors would like to thank the Department of Energy (DE-FG02-05ER64071 and DE-FG02-07ER46375) for their financial assistance.

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