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Advances in OptoElectronics
Volume 2011 (2011), Article ID 824927, 6 pages
Research Article

-Quantum-Dot Sensitized Metal Oxide Photoelectrodes: Photoelectrochemistry and Photoinduced Absorption Spectroscopy

1CRC, Department of Optometry, College of Applied Medical Sciences, King Saud University, P.O. Box 10219, Riyadh 11433, Saudi Arabia
2Department of Physical Chemistry, Uppsala University, P.O. Box 259, 75105 Uppsala, Sweden

Received 15 June 2011; Accepted 5 September 2011

Academic Editor: Surya Prakash Singh

Copyright © 2011 Idriss Bedja and Anders Hagfeldt. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.


TiO2, ZnO nanoparticulate(-np), and ZnO-nanorod(-nr) electrodes have been modified with FeS2 (pyrite) nanoparticles. Quantum size effect is manifested by a blue shift in both absorption and photocurrent action spectra. PIA (photoinduced absorption spectroscopy), a multipurpose tool in the study of dye-sensitized solar cells, is used to study quantum-dot modified metal oxide (MO) nanostructured electrodes. The PIA spectra showed an evidence for long-lived photoinduced charge separation. Time-resolved PIA showed that recombination between electrons and holes occurs on a millisecond timescale. Incident-photon-to-current efficiencies at 400 nm are ranged between 13% and 25%. The better solar cell performance of FeS2 on ZnO-nr over ZnO-np can be ascribed to the faster, unidirectional e-transport channels through the ZnO-nr as well as the longer electron lifetimes. The lower performances of electrodes can be explained by the presence of FeS2 phases other than the photoactive pyrite phase, as evidenced from XRD study.

1. Introduction

A great effort is being exerted to obtain efficient and inexpensive organic and inorganic solar cells. The approach of using semiconductor colloids for the design of optically transparent thin semiconductor films is considered as a unique and an alternative for the amorphous silicon solar cells. Under this approach, films made from colloidal metal oxide semiconductors which have large band gap have attained much attention. This is primarily because they are quite stable. In addition, they predominantly absorb in the UV region. The usefulness of these systems for solar cell applications was made possible by a basic principle, namely, sensitization of their semiconductor surfaces into visible region either by organic dyes (dye sensitization) [14] or by inorganic short band gap semiconductors also called quantum dots (QDs; semiconductor sensitization) [58]. Power conversion efficiencies in the range of 8–12% in diffuse daylight have been obtained in the ruthenium-based dye-sensitized highly porous TiO2 film [1]. On the other hand, wide band gap semiconductors have been sensitized by quantum dots, for example, CdSe/TiO2 [4] and CdS/TiO2-SnO2 [8] as alternative to dye sensitization. Vogel and coworkers [6] have investigated the sensitization of nanoporous TiO2, ZnO, and so forth by Q-sized CdS with the photocurrent quantum yields of up to 80% and open circuit voltages up to 1 V. In contrast with the dye sensitized solar cells, fundamental understanding of factors controlling the interfacial electron transfer reactions for the QD-sensitized solar cells is limited.

Dye sensitized solar cells (DSCs) based on one-dimensional (1D) ZnO nanostructures, which exhibit significantly higher electron mobility than that of both TiO2 and ZnO-np films [9], have recently been attracting increasing attention [9, 10].

In the present work, instead of organic dye as in DSCs, we used FeS2 quantum dot semiconductors to sensitize MO semiconductor thin films (MO = TiO2, ZnO-np, and ZnO-nr).

The FeS2 in pyrite phase is another favorable candidate of photosensitization materials because of its environmental compatibility, and high stability toward photocorrosion as well as its very good absorption in the visible region of the solar spectrum. The pyrite polymorph of iron disulfide is of particular interest, and shows promise for solar energy conversion devices in both photoelectrochemical and photovoltaic solar cells [11, 12] and solid-state solar cells [13] due to its favorable solid state properties [14]. Ennaoui et al. have reported interesting photoresponse of FeS2 modified polycrystalline TiO2 electrode [14] using CVD method. Shen et al. [15] have recently reported a method of modification of TiO2 large band gap (Degussa P25) by quantum-sized FeS2 particles by a similar procedure described originally by Chatzitheodorou et al. [16]. They reported only an incident-photon-to current efficiency of 25% at 400 nm excitation and an SEM picture of FeS2 adsorbed TiO2 film.

In this work, we report FeS2 QD sensitized TiO2, ZnO-np, and ZnO-nr photoelectrodes prepared by a method described previously by Shen et al. [15]. We described photoelectron-chemical properties and photoinduced absorption spectroscopy for mechanistic study.

2. Experimental

2.1. Preparation of Nanostructured Metal Oxide Film
2.1.1. TiO2 Nanoparticle Films

FTO plates are first put into a 0.02 M TiCl4 aqueous solution and kept at 70°C for 30 min. to obtain a thin dense layer of TiO2. A paste containing 20 nm sized TiO2 nanoparticles was subsequently spread on the substrate using a doctor blade method. Working electrodes were then sintered at 450°C for 30 min in a hot air stream.

2.1.2. ZnO Nanoparticle Films

The concentration of ZnO colloids was 0.05 M and was prepared by the method described by Spanhel and Anderson [9] with a little change. Addition of LiOH to the organometallic zinc complex solution was less by 25% than the required for stoichiometric addition. Colloidal ZnO solution thus obtained does not need any further concentration since small amount of solvent was used. The diameter of these colloidal particles was in the range of 2–5 nm. A small aliquot (0.1–0.8 mL) of ZnO sol was applied to the FTO substrate (  cm2). The films (0.5–3 μm) are dried in air and then heated at 400°C for 1 h. The sintered ZnO films adhered strongly to the FTO surface and were stable in neutral and alkaline solutions.

2.1.3. ZnO-Nanorod Films

Firstly, 300 nm ZnO seed layer was prepared on the FTO-coated glass. Two drops of 5 mM solution of zinc acetate dihydrate in absolute ethanol, rinsed in ethanol and blown dry with nitrogen gas. This is repeated 4 times before sintering at 350°C in air for 30 min. This process is repeated twice. Secondly, the thus ZnO-seeded substrate was immersed into an aqueous solution of 25 mM zinc nitrate hexahydrate, 25 mM hexamethylenetetramine and 5 mM polytheleneimine at 90°C for a chemical bath deposition during total 12 hours. The solution was replaced by a fresh one every 4 hours. The obtained ZnO nanorods were rinsed with deionized water and dried in air at room temperature.

2.2. Surface Modification of Metal Oxide Films by FeS2 Quantum Dots

FeS2 quantum dots were deposited onto nanostructured metal oxide films using a method to that described by Shen et al. [15], with a little modification. The metal oxide electrode was first dipped in a solution of 0.02 M sulfur in xylene, rinsed with xylene, and heated to 125°C for 5 min, followed by immersion in a solution of 0.01 M iron pentacarbonyl in xylene at a temperature of 139°C, followed by another xylene rinse and heating step (125°C). The whole experiment was carried out in a dry box under a nitrogen atmosphere. This procedure was repeated several times until the electrodes had become significantly darker in appearance.

2.3. Characterization Methods

UV-Vis spectra were recorded using an Ocean Optics HR2000 diode array spectrometer. Photoelectrochemical measurements were carried out using a potentiostat (Princeton Applied Research Model 273) with a 1 cm path-length quartz cuvette as the electrochemical cell. The FeS2-modified metal oxide electrode served as a working electrode, a Ag/AgCl (3 M KCl) as reference electrode, and a Pt wire as counter electrode. The electrolyte composition was Na2S 0.1 M and Na2SO4 0.01 M. The setups for recording incident photon to current efficiency (IPCE) spectra and I-V curves have been described elsewhere [17].

For PIA spectroscopy [18], excitation of the sample was provided by a blue LED (Luxeon Star 1 W, Royal Blue, 470 nm), which was square-wave modulated (on/off) by electronical means using an HP 33120A waveform generator and a home-built LED driver system. For the time-resolved studies the output of the current amplifier was connected to a data acquisition board (National Instruments, PCI-6052E). All PIA measurements were done at room temperature.

3. Results and Discussion

3.1. Characterization of FeS2-Modified Metal Oxide Electrodes

During deposition of FeS2 onto the metal oxide electrodes, the appearance of the metal oxide electrodes changed from white or transparent to a brown/grey color, which clearly indicates FeS2 adsorption as confirmed by the XRD study. Figure 1 shows XRD spectra of FeS2-modified metal oxides. Besides the sharp peaks assigned to SnO2 (cassiterite) from the FTO substrate and clear peaks from the metal oxide (ZnO wurtzite, TiO2 anatase), a number of much smaller and rather poorly resolved peaks also appeared. Possible origin of these peaks are FeS2 that exists in a cubic phase (pyrite: P) and an orthorhombic phase (marcasite: M). Furthermore hexagonal FeS (troilite) FeO, and so forth may also exist.

Figure 1: XRD spectra of FeS2 adsorbed metal oxide films. (a) ZnO-nr particulate film and (b) TiO2-nanoparticle film. A: anatase; P: pyrite, and M: marcasite.

The modified metal oxide electrodes were further analyzed using scanning electron microscopy. Figure 2(a) shows a cross section of a ZnO nanorod electrode before modification. The nanorods do not have a parallel orientation as a result of a nonoriented seed layer. The ZnO nanorods that were grown during 12 hours were about 8 μm in length and 300 nm in diameter. The inset clearly shows the deposition of a material in between the ZnO nanorods after the modification procedure. The deposited material, presumable FeS2, forms rather large aggregated structures. Figure 2(b) shows the top-view of mesoporous TiO2 films. The inset corresponds to modified TiO2 films which show formation of large FeS2 aggregates (sizes between 50–70 nm) on top of TiO2 nanoparticulate film with less uniformly distributed and dispersed.

Figure 2: Scanning electron microscope images of FeS2-modified and unmodified metal oxide electrodes. (a) Cross-section of a ZnO nanorod film. Inset: top view of an FeS2-modified ZnO nanorod film. (b) Top view of TiO2 nanoparticulate film. Inset: top view of TiO2 after FeS2 deposition.

UV-Vis absorption spectra (Figure 3) show that the deposited material absorbs light with wavelength lower than 600–700 nm. The low energy tail may come predominately from large particles. However, the high energy absorption shoulders are probably originated from ultrasmall particles. Because FeS2 has a small band gap around 1 eV [14], we would expect a large wavelength absorption onset near IR. Absorption spectra (Figure 3) show, however, particularly, short wavelength absorption onsets. This might be explained either in term of a quantum size effect of very small FeS2 particles which causes a band gap energy rising or simply because of nonstoichiometric pyrite present in the film. For this, the band gap of the material was analyzed by plotting (inset of Figure 3) the square root of the absorbance versus photon energy [19]. A linear relation was found for the square root of the absorbance, suggesting that the lowest band gap transition is indirect. The band gap, obtained by extrapolation, may vary between 1.6 and 2.0 eV depending on different metal oxide substrate. The reported value for the band gap of FeS2 is 0.95 eV [14]. This suggests that there is a strong quantum-size effect due to FeS2 particles.

Figure 3: Absorption spectra of FeS2 modified (a) ZnO-np, (b) ZnO-nr, and (c) TiO2-np particulate films. Inset: band gap determination from square root of absorbance spectra of FeS2-modified metal oxide electrodes: (a) ZnO-np, (b) ZnO-nr, and (c) TiO2-np particulate films.

Similarly, IPCE spectra (Figure 4) show essentially the same trend as the absorption spectra. The photoresponse of different metal oxide electrodes have been extended to the visible range after FeS2 modification. Although the FeS2/MO electrodes show strong visible absorption in wavelengths longer than 580 nm, no photoresponse was detected at these wavelengths. This suggests that only small quantum-sized FeS2 particles play a dominant role in the spectral sensitization on TiO2 particles while larger particles have less or no contribution. In order to validate the indirect band gap of FeS2 on different MO electrode, the material has been analyzed by plotting the square root of the IPCE versus photon energy (inset of Figure 4). Again, approximately linear relation was found for the square root of the IPCE, suggesting that the lowest band gap transition is indirect. The band gap, obtained by extrapolation, varied approximately between 1.5 and 1.9 eV.

Figure 4: IPCE spectra of FeS2 modified TiO2-np (filled triangle), ZnO-nr (filled square), and ZnO-np (filled circle). Inset is a band gap determination from square root of IPCE spectra of FeS2-modified metal oxide electrodes: (a) ZnO-np, (b) TiO2-np, and (c) ZnO-nr electrodes.

Photoinduced absorption (PIA) spectroscopy, where excitation is provided by an on/off modulated LED or laser giving intensities comparable to one sun is listed here under photoelectrochemical techniques, because it too allows for investigation of dye-sensitized (DSC) or quantum dots-sensitized (SSC) cells under actual operating conditions, and it can easily be combined with simultaneous electrochemical measurements [10, 20]. Small changes in optical transmission are detected using a detector system with a lock in amplifier tuned at the frequency of the modulation. It is very useful in qualitative studies, for instance, to check whether a dye or a quantum dot is injecting electrons into TiO2 after photoexcitation and whether a dye is regenerated when in contact with a redox electrolyte [21]. The kinetics of slower processes in the DSC or SSC can be followed using PIA. Because the PIA signal is proportional to the lifetime of the observed species, it can be sensitive to a small fraction of dye molecules that is not in contact with the redox couple or hole conductor and therefore has a long lifetime of the oxidized state [20].

PIA spectra in Figure 5 shows typical FeS2 modified different MO electrodes in the absence of the redox electrolyte (in air). The PIA spectra clearly reflect the differential spectrum of FeS2 upon formation of injected electrons into MO electrode (shown by absorption at large wavelengths), with a bleach of the main absorption of FeS2 around 470 nm and absorption peak at 580 nm (TiO2-np) and 670 nm (ZnO-nr). It has to be noted that no PIA spectrum for pyrite based ZnO-np photoelectrode has been recorded for comparison. This may be due to deep trapped electron sites and large number of boundaries in between ZnO nanoparticles which lead to a very low density of electrons that might leave and decay. For this case, only laser spectroscopy at high pulse intensity could detect that small intensity decay.

Figure 5: Photoinduced absorption spectra of FeS2 modified metal oxide electrodes in air: TiO2-np (filled triangle) ZnO-nr, (filled square), and ZnO-np (filled losange).

The PIA spectra indicate long-live charge separated state occurring in the Q-dot sensitized metal oxides: highest with FeS2 modified ZnO-nr.

3.2. PIA Kinetics

Study of the kinetics in semiconductor sensitizing solar cells is not only feasible by laser flash photolysis, a costly technique, but also possible using time-resolved PIA measurements. Figure 6 shows an example of such PIA transient; here decay recorded at 520 nm for FeS2 modified ZnO-nr slow on/off excitation; (pseudo-) first-order rate constant for bleach (growth at 520 nm) was estimated at about 0.15 ms, and is due to hole-electron recombination which also does not follow simple first-order kinetic as for TiO2-np modified with FeS2, but is characterized by a range of recombination times. This relatively fast decay also proves at least a well pore filling of ZnO-nr film by ultra fine particles of pyrite.

Figure 6: PIA decay transient absorption of Q-dots FeS2 modified ZnO-nanorod electrode after excitation with blue light of 11 mW/cm2 recorded at 520 nm using a sampling rate of 103 s−1 and averaged 100 times.

Similarly, Figure 7 shows PIA transient growth recorded at 800 nm for FeS2 modified TiO2-np. It is clear that the recombination yield between generated electrons and holes does not follow simple first- or even second-order kinetics, but is characterized by a range of recombination times. This has been explained by trapping of electrons within the TiO2 nanocrystals [20, 22]. Transport of electrons through TiO2 nanocrystals could also be one relation. For solar cell performance the (pseudo-) first-order rate constant under steady-state conditions is a relevant parameter as it can give direct information on possible recombination losses due to the reaction of electrons with holes. Analysis of the decay in Figure 6 during the first 1 ms (using a sampling rate of 1 MHz) gives a recombination lifetime of 6 ms. This relatively fast decay proves at least a well pore filling of TiO2 film by ultra fine particles of pyrite.

Figure 7: PIA decay transient absorption of Q-dots FeS2 modified TiO2 electrode after excitation with blue light of 11 mW/cm2 recorded at 800 nm using a sampling rate of 103 s−1 and averaged 100 times.

4. Conclusion

The pyrite of iron disulfide (FeS2) shows promise for solar energy conversion devices in photoelectrochemical solar cells. FeS2 can be used to sensitize different types of metal oxides. Indirect band gap has been determined for FeS2 modified MO electrodes. Low performance of the electrodes is mainly due to the presence of multiphase FeS2. Looking for a pure and stoichiometric pyrite will be very promising for solar cells based on quantum dots semiconductors.


The research project is funded by the National Plan for Science and Technology Program, Grant number 09-NAN859-02, King Saud University, Riyadh, Saudi Arabia. I. Bedja would like to thank Dr. Gerrit Boschloo for his helpful discussions.


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