International Journal of Photoenergy

International Journal of Photoenergy / 2010 / Article
Special Issue

Thin-Film Photovoltaics

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Research Article | Open Access

Volume 2010 |Article ID 497095 |

Ming-Hong Lai, Auttasit Tubtimtae, Ming-Way Lee, Gou-Jen Wang, "ZnO-Nanorod Dye-Sensitized Solar Cells: New Structure without a Transparent Conducting Oxide Layer", International Journal of Photoenergy, vol. 2010, Article ID 497095, 5 pages, 2010.

ZnO-Nanorod Dye-Sensitized Solar Cells: New Structure without a Transparent Conducting Oxide Layer

Academic Editor: Gaetano Di Marco
Received24 Nov 2009
Accepted21 Dec 2009
Published17 Mar 2010


Conventional nanorod-based dye-sensitized solar cells (DSSCs) are fabricated by growing nanorods on top of a transparent conducting oxide (TCO, typically fluorine-doped tin oxide—FTO). The heterogeneous interface between the nanorod and TCO forms a source for carrier scattering. This work reports on a new DSSC architecture without a TCO layer. The TCO-less structure consists of ZnO nanorods grown on top of a ZnO film. The ZnO film replaced FTO as the TCO layer and the ZnO nanorods served as the photoanode. The ZnO nanorod/film structure was grown by two methods: (1) one-step chemical vapor deposition (CVD) (2) two-step chemical bath deposition (CBD). The thicknesses of the nanorods/film grown by CVD is more uniform than that by CBD. We demonstrate that the TCO-less DSSC structure can operate properly as solar cells. The new DSSCs yield the best short-current density of 3.96 mA/ and a power conversion efficiency of 0.73% under 85 mW/ of simulated solar illumination. The open-circuit voltage of 0.80 V is markedly higher than that from conventional ZnO DSSCs.

1. Introduction

Dye-sensitized solar cells (DSSC) are a promising low-cost, green energy source [1, 2]. A power conversion efficiency of 11.18% has been achieved in 2005 [3]. The high efficiency of DSSCs can be attributed to the structure of a photoelectrode which consists of a layer of nanoparticle TiO2 sintered to a transparent-conducting oxide (TCO). The mesoporous TiO2 nanoparticles increase the surface area for dye chemisorptions to a thousand folds over that of a flat electrode of the same size [4]. The progress in enhancing the performance of DSSCs has been slow over the last decade. One of the main problems is the limited diffusion length of the photogenerated electrons. The photogenerated carriers conduct via random hopping through a percolated path in a three-dimensional network of nanoparticles. Previous studies have shown that the photogenerated carriers must undergo 103–106 hoppings (trapping and detrapping) before they reach the collecting electrodes [5]. Carrier trapping, presumably by defect states at the surface of nanoparticles [6, 7], leads to a low electron diffusion coefficient () [8], which is several orders of magnitude smaller than that of single-crystal [9].

To improve the electron transport, researchers have tried to design DSSCs without a nanoparticulate structure. One promising approach is to replace the nanoparticles with crystalline TiO2 nanorods (or nanowires, nanotubes), thereby eliminating the grain boundaries between nanoparticles. TiO2-nanorod DSSCs have yielded recombination time constants an order of magnitude longer and significantly higher charge-collection efficiencies than that of nanoparticulate DSSCs [10, 11].

Work on nanorod-based DSSCs has been based on the system [12, 13], although recently the ZnO system has also started to attract more attention [14, 15]. ZnO has an energy gap of 3.37 eV, nearly identical to that of TiO2. Currently, ZnO nanorod arrays are grown on a TCO glass (fluorine-doped tin oxide—FTO). A disadvantage in this structure is that a heterogeneous interface exists between the FTO glass and the nanorods, which forms a source for electron scattering.

To increase the conversion efficiency of nanorod-based DSSCs, it would be desirable to eliminate the interface between FTO and the ZnO nanorods. Replacing the FTO layer with a ZnO film could eliminate the heterogeneous interface. Further more, since ZnO is transparent to the whole visible spectrum, it is a good TCO material. Chen et al. have recently carried out this concept by growing ZnO nanorods on a ZnO film using a two-step method [16]. In this work we grew ZnO nanorods on a ZnO film using two different techniques: one-step chemical vapor deposition (CVD) and two-step chemical bath deposition (CBD). The photovoltaic properties of the TCO-less DSSC samples were systematically investigated. The results were compared to those of a conventional ZnO-nanorod DSSC (i.e., ZnO nanorods grown on an FTO film). The electron transport characteristics were analyzed using the one-diode circuit model.

2. Experimental Procedure

2.1. Sample Growth
2.1.1. CVD Growth

In the first experiment we grew ZnO nanorods on a ZnO film using the one-step CVD technique. High-purity Zn slugs (6N) were placed on an alumina boat inside a quartz one-inch diameter tube in a furnace. The c-plane (0001) sapphire single-crystalline substrates were placed 7 cm downstream from the Zn source. The growth conditions were: temperature 850–900°C and gas flow rates: 2 sccm (O2) and 15 sccm (Ar), and growth time: 35 min. In the first stage of the growth process, a ZnO film grew on the sapphire substrate; in the second stage, ZnO nanorods started to grow on top of the ZnO film. The grown samples were examined by a scanning electron microscope (SEM). Photoluminescence (PL) spectra were measured using an HeCd laser of 325 nm wavelength.

2.1.2. CBD Growth

The second sample growth experiment employed a two-step CBD method. In the first step, a ZnO film was grown on a glass substrate; in the second step, ZnO nanorod arrays were synthesized on top of the ZnO film. The substrates were Corning 1737 glass. Aqueous solutions of 0.08 M of zinc nitrate hexahydrate and 0.05 M of hexamethylenetetramine C6H12N4 (HMT) were used as the precursors for the ZnO films. One M of hydrogen peroxide (H2O2) was added to the solution to make it more turbid (pH 6.0–6.5), which is advantageous for obtaining more uniform thin films. A layer of ZnO film was deposited on the substrate after the reaction at 90°C for 1.3 h. For the growth of ZnO nanorods, the ZnO film-coated substrate was immersed vertically in a beaker containing a 0.01 M solution of the precursors used in the first step (zinc nitrate hexahydrate and HMT). The reaction was carried out at 95°C for 5 h. The process was repeated five-to-six times in order to obtain higher density and longer nanorods.

2.1.3. Growth of ZnO Nanorods for Conventional DSSCs

For comparison, a third reference sample was grown by the CBD method. The sample had the structure of conventional DSSCs—ZnO nanorods grown on an FTO glass substrate. Prior to the growth, a seed layer of ZnO nanoparticles was first deposited by immersing an FTO substrate into a solution of 0.5 M zinc acetate and HMT for 30 min. ZnO nanorods were then grown on the substrate using the CBD method. The growth conditions were identical to those in Section 2.1.2.

2.2. Fabrication of Solar Cells

The TCO-less ZnO DSSCs were fabricated as follows. The ZnO film/nanorod sample was sensitized by immersion in a solution of  M N719 dye for 24 h at room temperature. An FTO glass with Pt foil 150 m in thickness served as the counter electrode. The ZnO electrode and the counter electrode were assembled and sealed by a 25 m thick parafilm spacer. The electrolyte was composed of 0.5 M LiI, 0.05 M I2, 0.5 M 4-tert-butylpyridine, and 0.6 M 1-butyl-methylimidazoilium iodide in acetonitrile and valeronitrile. Figure 1 shows the schematic structure of a fabricated TCO-less DSSC on the grown ZnO film/nanorods.

2.3. Photovoltaic Measurements

The current-voltage (I-V) characteristics measurements were performed using a 150 W Xe lamp (Oriel). A filter was placed in front of the sample to simulate the AM 1.5 spectrum. The active area of the cell was .The photocurrent was recorded using a Keithley 2400 sourcemeter. The conversion efficiency is calculated as follows: , where (mA/cm2) is the short-circuit current density, is the open-circuit voltage, FF is the fill factor, and (mA/cm2) is the intensity of the incident light.

3. Results and Discussion

3.1. Structure Characterization

Figure 2 shows (a) top view, (b) cross-sectional SEM images of ZnO nanorods on a ZnO film grown by the one-step CVD method. The nanorods have an average length of 20 m, diameter ranging from 100 to 200 nm and they are mostly vertically aligned with the substrate. A ZnO film of thickness 2 m can be clearly seen. Figure 3 shows a SEM image of ZnO nanorods grown by the two-step CBD method. The nanorods have diameters ranging from 50 to 500 nm and length from 7 to 10 m. The ZnO film has a thickness ranging from 0.3 to 1 m. It can be seen that the CVD-grown nanorods have a more uniform distribution in thickness than that in the CBD sample. The thickness of the CVD-grown ZnO film is also more uniform.

Figure 4 shows the X-ray diffraction patterns of the ZnO film/nanorods grown by the three methods. The diffraction patterns correspond to the hexagonal wurtzite structure with lattice constants of a = 3.176 Å, c = 5.187 Å. In the CVD sample, the most pronounced peak is (002), indicating that the preferential growth is along the c axis of a nanorod. In contrast, the diffraction pattern of the conventional ZnO sample shows the main (002) peak along with many weak peaks, indicating no preferential orientation in the nanorod growth. The difference in nanorod orientation is an effect of the substrate. In the CVD growth, single-crystalline sapphire was used, resulting in oriented nanorods. In the conventional method, FTO glass without preferential orientations was used, resulting in randomly orientated nanorods.

Figure 5 shows the room-temperature PL spectra of ZnO nanorods grown by the CVD and CBD methods. The CVD sample shows a sharp blue peak at  nm, attributed to the free exciton emission of ZnO. In the CBD sample this blue peak is upshifted to 353 nm and a broad peak at 430 nm is observed. The latter peak can be attributed to singly ionized oxygen vacancies [17]. We observed that CVD processing in a lower oxygen partial pressure led to more oxygen vacancies and a larger 430 nm peak.

3.2. Photovoltaic Properties

Figure 6 shows the photocurrent-voltage (I-V) characteristics for three ZnO-nanorod DSSC samples grown by the CVD, CBD and conventional methods. The photovoltaic characteristics are listed in Table 1. The CVD-grown sample has an open circuit voltage of 0.80 V and an energy conversion efficiencyη = 0.73%. The CBD sample has a higher short-circuit current density of mA/cm2. The efficiency is very close to that of Chen et al. (0.77%) for a DSSC with the same TCO-less structure. The conventional DSSC has a conversion efficiency of %. In general, the energy conversion efficiency of ZnO DSSCs is lower than that of TiO2 DSSCs. Note that the efficiency of ZnO-nanorod-based DSSCs is typically 1%-2% [18].

Sample (V) (mA/cm2)FF (%)η (%)


A notable feature of the present result is that the open-circuit voltage of the TCO-less DSSCs is relatively high (0.80 V), about 20%–40% higher than that of conventional ZnO-nanorod DSSCs, typically 0.6 V [19, 20]. According to the kinetic model, the open-circuit voltage is limited by -, where is the Fermi level of ZnO and is the redox potential of the electrolyte. The actual obtained in experiments is lower than the theoretical upper limit due to the dark current in the solar cell. The dark current is mainly caused by carrier recombination between the photoinjected electrons in the semiconductor and the positively charged dye molecules or electrolyte. Our present result suggests that carrier recombination in the TCO-less structure is reduced, resulting in a larger .

The conversion efficiencies of the TCO-less DSSCs are lower than those of the conventional DSSC. We attribute this to the large resistance in the ZnO film. We analyze the series resistance and shunt resistance of the DSSC from I-V curve using the one-diode model. The equivalent circuit is shown in Figure 7. The equation of the circuit is

where is the photo current, is the diode current, is the shunt current, is the initial current, n is the diode factor, q the electric charge, and k is the Boltzmann constant. The I-V curve (a) in Figure 6 (the CVD sample) was taken for fitting. The best fit yields the parameters:  mA/cm2,  nA/cm2,  Ω, and  kΩ. Considering recombination current in DSSCs, the diode factor n was set to 2 in the fitting. The series resistance is relatively large for solar cells, which is because the ZnO film is undoped and, therefore, has a large resistance. Doping to the film with Ga or In should produce a lower-resistance film, which will increase the efficiency of the DSSCs.

The one-step growth method in the present work has several advantages over Chen’s two-step MOCVD method. In Chen’s method, a Ga-doped ZnO film was grown on the substrate in the first step; ZnO nanotips were grown on top of the ZnO film in the second step. The experimental conditions had to be varied during the two steps. In the present work, a one-step vapor-transport CVD method was used to grow the ZnO film/nanorod structure. The sample growth could be completed in one run. The new method is simpler, reaction time is shorter, and the growth equipment is much cheaper than MOCVD.

4. Conclusion

In conclusion, we have demonstrated a new DSSC structure without a TCO layer. A ZnO film, grown by the one-step CVD or the two-step CBD method, is used to replace the TCO layer. The new structure eliminates the interface between the nanorod and the TCO film. The ZnO nanorods and ZnO films grown by the CVD method have more uniform thickness. The DSSC structure yields an open-circuit voltage markedly higher than that from DSSC on an FTO glass. Higher electrical conductance in the ZnO film is needed to improve the DSSC efficiency.


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Copyright © 2010 Ming-Hong Lai et al. 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.

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