Xiao Hua Yang‡
a,
Ling Cheng‡a,
Yu Houa,
Bo Zhangab,
Long Wua and
Hua Gui Yang*ac
aKey Laboratory for Ultrafine Materials of Ministry of Education, School of Materials Science and Engineering, East China University of Science & Technology, Shanghai 200237, China. E-mail: hgyang@ecust.edu.cn; Fax: +86-21-64252127
bDepartment of Physics, East China University of Science and Technology, 130 Meilong Road, Shanghai 200237, China
cCentre for Clean Environment and Energy, Gold Coast Campus, Griffith University, Queensland 4222, Australia
First published on 17th February 2014
The electrocatalytic behavior of the Fe2O3, In2O3 and SnO2 counter electrodes prepared in H2 is enhanced significantly. This work demonstrated that hydrogen-treatment is a facile and universal method for the preparation of efficient electrocatalysts in dye-sensitized solar cells.
Recently, we have demonstrated that the low-cost commercial tungsten oxide (WO3) with thermal treatment in hydrogen atmosphere presented an 800% enhancement of energy conversion efficiency of the DSCs.19 The oxygen vacancies introduced in material surface during the hydrogen treatment demonstrate its capacity for the improvement of electric conductivity and catalytic activity of the WO3 as the CE material.20 Therefore, this realistic approach is expected to be effective in increasing the energy conversion efficiency for various metal oxides with substoichiometric surface, as presented in the hydrogen-treated WO3. Herein, in this work, we randomly choose three commercial transition-metal oxides (Fe2O3, In2O3 and SnO2), and systematically analyze the electrocatalytic performance of the pristine commercial oxides (C–Fe2O3, C–In2O3 and C–SnO2) and corresponding hydrogen-treated ones (H–Fe2O3, H–In2O3 and H–SnO2). The energy conversion efficiency of the DSCs with different hydrogen-treated transition-metal oxides as CEs, predictably, would be much higher than the corresponding value of the commercial ones with stoichiometric surface.
Fig. 1 displays the photocurrent–voltage (J–V) curves for the DSCs with different CEs, and the detailed photovoltaic parameters are summarized in Table 1. The DSCs using commercial CEs showed very low energy conversion efficiencies of 1.13% for C–Fe2O3, 1.15% for C–In2O3 and 0.83% for C–SnO2. In contrast, the DSCs using hydrogen-treated CEs exhibited high energy conversion efficiencies of 6.05% for H–Fe2O3, 5.84% for H–In2O3 and 3.05% for H–SnO2, giving improvements of 535%, 509% and 476%, respectively. Aside from the energy conversion efficiency, the short-circuit photocurrent density (Jsc), open-circuit voltage (Voc) and fill factor (FF) of DSCs are all increased remarkably, which means that the hydrogen-treated CEs have a higher electrical conductivity and a better electrocatalytic activity towards I3−/I− redox pairs. These interesting results may be attributed to the introduced oxygen vacancies during hydrogen treatment. Thus, it can be concluded that the hydrogen treatment is an efficient method for introducing oxygen vacancies to obtain highly active oxide CE materials.
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Fig. 1 J–V curves of DSCs with different CEs: C–Fe2O3, H–Fe2O3, C–In2O3, H–In2O3, C–SnO2 and H–SnO2. |
Samples | Jsc (mA cm−2) | Voc (mV) | FF (%) | η (%) |
---|---|---|---|---|
H–Fe2O3 | 17.92 | 670 | 50 | 6.05 |
C–Fe2O3 | 11.90 | 500 | 19 | 1.13 |
H–In2O3 | 14.97 | 710 | 55 | 5.84 |
C–In2O3 | 10.82 | 550 | 19 | 1.15 |
H–SnO2 | 16.32 | 725 | 26 | 3.05 |
C–SnO2 | 11.53 | 550 | 13 | 0.83 |
To further confirm that the high catalytic activity of the hydrogen-treated CEs is caused by the introduction of oxygen vacancies, systematic characterizations were performed by using C–Fe2O3 and H–Fe2O3 as the examples. It is well known that the electrochemical impedance spectroscopy (EIS) is an effective and widely used method to examine the electrochemical characteristics and thereby to evaluate the catalytic activity of a catalyst. EIS measurement was carried out with symmetric cells fabricated with C–Fe2O3 and H–Fe2O3 as CEs, respectively. The results are shown in the form of a Nyquist plot (Fig. 2a). The equivalent circuit used to fit the experimental EIS data is shown in the inset of Fig. 2a. The high-frequency intercept on the real axis represents the series resistance (Rs), which is mainly composed of the bulk resistance of CEs materials, resistance of FTO glass substrate, contact resistance, etc.21 As expected, the Rs values of the H–Fe2O3 CE (16.0 Ω) is lower than that of the C–Fe2O3 CE (17.7 Ω), which indicated that H–Fe2O3 CE has a better electrical conductivity than C–Fe2O3 CE, and is also consistent with the tendency of the observed Jsc. The smaller Rs might be attributed to the positively charged oxygen vacancies which can greatly improve electron transfer by trapping electrons. The semicircle on the left side represents the Rct which reflects the electrocatalytic activity of the CE materials for the reduction of triiodide ions.22 The Rct value of H–Fe2O3 CE (3.25 Ω) is much smaller than that of C–Fe2O3 CEs (4.51 Ω), which means H–Fe2O3 has a better catalytic activity. These EIS results demonstrate that H–Fe2O3 behaves better than C–Fe2O3 as a CE catalyst for the triiodide reduction.
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Fig. 2 EIS (a) and CV (b) of DSCs with C–Fe2O3 (black line) and H–Fe2O3 (red line) CEs, respectively. |
To further evaluate the electrocatalytic properties of the as-prepared H–Fe2O3, cyclic voltammetry (CV) was carried out in a three-electrode system (see Fig. 2b). The CV curves of H–Fe2O3 show two well-defined reduction peaks and the corresponding oxidation peaks for each electrode. The pair of peaks at low potential correspond to the redox reaction shown in eqn (1), and the pair at high potential correspond to the redox reaction shown in eqn (2).23
I3− + 2e = 3I− | (1) |
3I2 +2e = I3− | (2) |
As shown in Fig. 2b, compared to the CV curve for C–Fe2O3 electrode, H–Fe2O3 has relatively higher current densities, suggesting the redox reaction of I3−/I− has been greatly enhanced on the surface of H–Fe2O3 electrode, which produces favorable conditions for the regeneration of the sensitizer. The CV result confirms again that the H–Fe2O3 have a superior electrocatalytic activity in reducing triiodide, which is in accordance with the results of EIS analysis.
To check the morphologies and crystal structures of the C–Fe2O3 and H–Fe2O3, scanning electron microscopy (SEM) and X-ray powder diffraction (XRD) measurements were carried out. The SEM image (Fig. 3a) shows that H–Fe2O3 is formed in variably size blocks ranged from 100 nm to 500 mm and compared to the original C–Fe2O3 sample (ESI Fig. S1†). There is no obvious change observed in the size and morphology. As shown in Fig. 3b, the most intensive diffraction peaks of C–Fe2O3 match well with the typical hematite Fe2O3, which are shown at the bottom of the Fig. 3b. There is no obvious shift of the diffraction peaks accompanied with the emergence of some new peaks in the H–Fe2O3 sample. These new peaks (highlighted by * in Fig. 3b) may be indexed to iron and ferroferric oxide, confirming the successful reduction of Fe2O3. Compared to the C–Fe2O3, the diffraction peaks of H–Fe2O3 sample gradually disappear, while the (110) diffraction peak is more stronger. The (110) diffraction peak suggests that H–Fe2O3 have a preferred [110] direction on the substrate, which means that they were grown along the [110] axis. The conductivity of hematite along the [110] axis is four orders of magnitude higher than the [001] direction because of a hopping mechanism related to Fe2+/Fe3+ mixed valence states.24
To further determine the effect of hydrogen treatment on the surface structure of Fe2O3, X-ray photoelectron spectroscopy (XPS) was performed to obtain Fe 2p core-level XPS spectra (Fig. 4). Typical Fe 2p peaks can be observed at 722.8 and 709.5 eV with a shake-up satellite line at 717.3 eV, which is generally assigned to Fe3+ in Fe2O3 and Fe3O4.25 In addition, the H–Fe2O3 sample exhibits an obvious satellite peak around 713.1 eV corresponding to Fe2+,26 implying the existence of Fe2+ (oxygen vacancies) sites which lead to a better catalytic activity. The oxygen vacancies can serve as shallow electron donor to greatly facilitate the electrons migration. Moreover, oxygen vacancies may act as the active sites for absorbing I3− and catalyzing its reduction for generating I−.
Footnotes |
† Electronic supplementary information (ESI) available: Experimental details, SEM image. See DOI: 10.1039/c3ra46109b |
‡ These authors contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2014 |