International Journal of Photoenergy

Volume 2013 (2013), Article ID 807931, 6 pages

http://dx.doi.org/10.1155/2013/807931

Research Article

Integration of High-Performance Nanocrystalline TiO₂ Photoelectrodes for N719-Sensitized Solar Cells

Ke-Jian Jiang,¹ Jin-Ming Zhou,¹ Kazuhiro Manseki,² Qi-Sheng Liu,¹ Jin-Hua Huang,¹ Yan-lin Song,¹ and Shozo Yanagida³

¹Laboratory of New Materials, Institute of Chemistry, Chinese Academy of Sciences, Beijing 100190, China

²Graduate School of Engineering, Environmental and Renewable Energy System (ERES) Division, Gifu University, 1-1, Yanagido, Gifu 501-1193, Japan

³ISIR, Osaka University, 2-1, Mihoga-oka, Ibaraki, Osaka 567-0047, Japan

Received 12 February 2013; Accepted 21 April 2013

Academic Editor: Theodoros Dimopoulos

Copyright © 2013 Ke-Jian Jiang 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.

Abstract.

We report on enhanced performance of N719-sensitized TiO₂ solar cells (DSCs) incorporating size and photoelectron diffusion-controlled TiO₂ as sensitizer-matched light-scatter layers on conventional nanocrystalline TiO₂ electrodes. The double-layered N719/TiO₂ composite electrode with a high dye-loading capacity exhibits the diffused reflectance of more than 50% in the range of  = 650–800 nm, even when the films are coupled with the titania nanocrystalline underlayer in the device. As a result, the increased near-infrared light-harvesting produces a high light-to-electricity conversion efficiency of over 9% mainly due to the significant increase of . Such an optical effect of the NIR-light scattering TiO₂ electrodes will be beneficial when the sensitizers with low molar extinction coefficients, such as N719, are introduced in the device.

1. Introduction

Dye-sensitized solar cells (DSCs) have been explored from both academic and industry world as a promising alternative to the conventional silicon-based photovoltaic devices [1–3], and efficiencies of over 12% have been achieved [4]. In this cell, a wide band-gap nanostructured semiconductor electrode (typically, TiO₂) is employed to support a large surface area, on which dye molecules are assembled to improve the light harvesting of the dyed electrode. A great deal of effort has been focused on the development of effective panchromatic sensitizers or cosensitizers for efficient solar light harvesting in DSC devices. On the other hand, the light-harvesting efficiency of DSC can be promoted by introducing a sophisticated structure in the photoelectrode, in which the photon path length is increased by the confinement of incident solar energy light. Usami made the theoretical finding that lightscattering in DSCs will be optimized if the diameter of TiO₂ nanocrystals is twice the size of the wavelength of incident light [5]. The effect has been verified in the DSCs, in which a TiO₂ layer built from submicrometer-sized TiO₂ particles was employed in combination with a transparent nanostructured TiO₂ layer [6–8]. In addition, TiO₂ (or ZnO) photoelectrodes with submicrometer-sized beads, hollow spheres, and tubes have been widely investigated [9–15].

As an alternative to such a large particle light-scattering material, TiO₂ layers with periodic pore structures exhibiting photonic band gaps have been applied for DSCs to enhance light harvesting efficiency [16–21]. Such light scattering TiO₂ layers, however, required an elaborate multistep synthesis. On the other hand, Hore et al. reported scattering of light on disordered spherical voids in TiO₂ electrodes for enhanced DSC performance. The DSC with 400 nm void layers gave a higher efficiency (6.7%) as compared to the cavity-free layer (5.4%) [22]. While the overall efficiency was improved, a slight increase of was observed and the appreciable increase of fill factors resulted in the 18% increment of conversion efficiency. Despite a number of nanostructured TiO₂ photoelectrodes reported as mentioned previously, the cell performance originated from spherical void-centered TiO₂ has still been poorly understood. Most importantly, little has been reported on an enhancement of near-infrared-(NIR-) light response in IPCE [22, 23]. As organic dye molecules with large extinction coefficients even in the red region were used, the results represent a compromise between slight light scattering and enhanced mobility of viscous electrolytes in the large hollow cavities [23]. In this paper we demonstrate optimized effects of scattering on submicron TiO₂ particles with spherical cavities on quantum efficiencies of light-to-electricity conversion of N719-sensitized solar cells at a NIR region, where the N719 dye has a low extinction coefficient. Accordingly, we prepared a TiO₂ layer containing 600 nm large spherical cavities and combined successively with the conventional nanocrystalline TiO₂ layer. We then applied the hollow-cavity-based TiO₂/nanocrystalline TiO₂ double composite electrodes to N719-sensitized DSC. The DSC exhibited a maximum conversion efficiency of 9.25% versus 6.38% for the reference cell with single conventional TiO₂ electrodes. We demonstrated that the hollow-cavity-based TiO₂ contributes not only to the enhanced absorption of near-infrared photons but also to effective dye sensitization as evidenced by the remarkable enhancement of in the performance. It should be noted that the effective electron diffusion coefficient of the dye-coated light-scattering TiO₂ layer also plays a crucial role in the improved DSC performance.

2. Materials and Methods

Polyethyleneglycol (PEG, ) was purchased from Fluka Co. The Ru dye, N719 (cis-bis(isothiocyanato) bis(2,2′-bipyridyl-4,4′-dicarboxylato)-ruthenium (II) bis-tetrabutylammonium) was purchased from Solaronix S.A. Iodine, 1-propyl-3-methylimidazolium iodide, valeronitrile, lithium iodide, and tert-butylpyridine were purchased from Aldrich without purification.

2.1. Preparation of DSCs

A 60 nm dense TiO₂ layer was deposited on a patterned ITO-coated glass substrates (10 Ω/□, Nippon Sheet Glass) by spin coating technique with tetraisopropyl orthotitanate in ethanol, as reported previously [24]. The TiO₂ films, served as a blocking layer in DSCs, were annealed in air at 500°C for 30 minutes. Following this, a TiO₂ paste with 20 nm particle size was deposited by doctor blade technique on the blocking layer, where the TiO₂ paste was prepared according to the previous report [25]. A transparent TiO₂ underlayer was achieved after the calcination at 500°C for 30 minutes. Functional polystyrene spheres (PS) (560 nm in size) were synthesized according to our previous method [26]. The resulting latex spheres were used directly without purification. The polystyrene spheres (PS) were fabricated via batch emulsion polymerization, where styrene was mixed with methyl methacrylate (MMA) and acrylic acid (AA). For the preparation of the spherical cavity-based light-scattering TiO₂ layer, as prepared spheres were dispersed in the TiO₂ colloid with the particle size of about 20 nm as a coating paste for the preparation of the overlayer. The PS sphere, the previously mentioned TiO₂ colloid, and PEG were mixed in water with ratio of 1/0.5/0.3 (TiO₂/PS/PEG, by weight) and homogenized with a stirring bar and ultrasonication. The resulting paste was deposited as a light-scattering layer on the underlayer, followed by the same calcination procedure mentioned previously. Finally, the double-layered TiO₂ film was impregnated with 0.2 M TiCl₄ aqueous solution at room temperature overnight and then calcinated again at 500°C for 30 minutes. After cooling to about 120°C, the films were emerged overnight in 1 : 1 v/v acetonitrile and tert-butyl alcohol solvent mixture containing N719 dye at a concentration of 0.3 mM. A Pt-sputtered FTO glass was used as a counter electrode. The electrolyte was composed of 0.6 M 1-propyl-3-methylimidazolium iodide, 0.1 M LiI, 0.04 M I₂, and 0.5 M tert-butylpyridine in the mixture of acetonitrile and valeronitrile (1 : 1, by volume).

2.2. Characterization and Photoelectric Measurements

The SEM images of titania films were obtained with a field-emission SEM (JEOL JSM-4800, Japan). The optical reflection measurement was performed using an UV-vis spectrophotometer (U-3010, HITACHI) equipped with an integrating sphere.

The incident photon-to-current conversion efficiency (IPCE) for solar cells was measured by using a commercial setup (PV-25 DYE, JASCO) equipped with a monochromator. A 300 W Xenon lamp was employed as a light source for the generation of a monochromatic beam. Calibrations were performed with a standard silicon photodiode. IPCE is defined by , where is Planck’s constant, is the speed of light in a vacuum, is the electronic charge, is the wavelength in meters (m), is the short-circuit photocurrent density (A m⁻²), and is the incident radiation flux (W m⁻²). The photocurrent-voltage (I-V) characteristics were recorded using a computer-controlled Keithley 2400 source meter under air mass (AM) 1.5 simulated illumination (100 mw cm⁻², Oriel, 67005). The active area of the samples was about 0.2 cm², controlled by an aperture mask to prevent extra light from coming through the lateral space. I-V data were well within experimental error.

3. Results and Discussion

As shown in Figure 1(a), the latex PS sphere holds a hard PS core with an elastomeric PMMA/PAA shell and presents a monodispersity with the size of about 560 nm (Figure 1(b)). The TiO₂ overlayer was prepared through a simple mixing of submicrometer-size polystyrene (PS) spheres and nano sized TiO₂ particles, followed by subsequent coating and calcinations on a transparent TiO₂ underlayer. The PS spheres vanish during the calcination process.

(a)

(b)

Figure 1: (a) A schematic structure of the functionalized polystyrene spheres. (b) A SEM image of the PS spheres with a diameter of 560 nm.

The SEM image in Figure 2(a) shows a top surface image of the TiO₂ overlayer. It is very clear that homogeneous spherical voids spread on the whole surface with the size of around 600 nm. Figure 2(b) shows a top surface image of the TiO₂ transparent layer, which presents a porous structure comprised of 20 nm sized TiO₂ particles. The cross-sectional image of the corresponding double-layer electrode is shown in Figure 2(c), where the 8 µm thick transparent nanoporous TiO₂ underlayer and the 6 µm thick TiO₂ overlayer are formed without cracks.

(a)

(b)

(c)

Figure 2: Scanning electron micrographs of (a) the top view of a spherical-cavity-based TiO₂ film, (b) the top view of a nanocrystalline TiO₂ film, (c) cross-sectional view of the double-layer TiO₂ film with a nanocrystalline TiO₂ layer and a spherical-cavity-based TiO₂ layer.

In order to investigate the light-scattering ability of the overlayer, UV-vis reflectance spectra were recorded for a 6 µm thick spherical-cavity-based TiO₂ film with and without sensitization by using a standard N719 dye, and an 8 µm-thick nanostructured TiO₂ film was employed for comparison, as shown in Figure 3. For the film without the dye loading, the reflectance of the overlayer is more than 70% in the whole UV-vis region, indicating that more than 90% of the light reflecting efficiency can be achieved by the overlayer when considering the absorption and reflection by the FTO glass substrate. By contrast the reflectance of the transparent nanostructured TiO₂ underlayer is less than 30%. After the dye adsorption, the reflectance was significantly decreased in the spectral range by around 535 nm for both the layers, where N719 dye has the maximum absorption, indicating that the reduction is mainly ascribed to the light absorption by the dye. Most importantly, the diffused reflectance of the TiO₂/dye composite film is found to be more than 50% in the range of   =  650–800 nm after the dye loading for the overlayer.

(a)

(b)

Figure 3: Diffused reflectance spectra of a nanocrystalline TiO₂ film (8 µm thick) and a spherical-cavity-based TiO₂ film (6 µm thick) without (a) and with (b) N719 dye loading.

We tested the double composite films as DSC photoelectrodes (denoted as sample 1) consisting of a 8 µm thick nanostructured TiO₂ underlayer and a 6 µm thick overlayer, in which a single-layer TiO₂ electrode only with the 8 µm thick TiO₂ underlayer (sample 2) was used for comparison. The current-voltage characteristics are shown in Figure 4 and Table 1. The conversion efficiency () was improved from 6.38% for sample 2 to 9.25% for sample 1, corresponding to the 45% increment. The improved efficiency was mainly caused by the increase of the short-circuit current density () from 13.04 mA cm⁻² to 18.40 mA cm⁻², while the and fill factors are the same or comparable for the two samples. It should be noted that, in the overlayer, the submicro-meter sized voids are surrounded by the nanostructured TiO₂ film with the TiO₂ particles of 20 nm. The dye molecules can be absorbed on the overlayer to contribute to the increment of in the double layer. In order to evaluate the effect of dye absorption in the overlayer on , the one-layer nanostructured TiO₂ electrode with a thickness of 10 µm was prepared (sample 3), by considering the amount of the dye loading for fair comparison (the porosity of TiO₂ overlayer : ~80%). The amounts of the absorbed dyes were determined for the three different electrodes by measuring the eluted dye concentration from the TiO₂ electrodes as shown in Table 1. The dye adsorption capacity was comparable for samples 1 and 3, suggesting that the scattering layer maintains a high dye-adsorption capacity. As shown in Table 1, sample 3 with the 10 µm thick TiO₂ electrode gave 14.86 mA cm⁻² of , which was much lower than that of sample 1. A further comparison between sample 2 and sample 3 showed only a slight increase (1.82 mA cm⁻²) in . On the other hand, the reflectance for sample 1 was significantly higher across the visible part of the spectrum than that of a single-layer TiO₂ cell as mentioned previously. Therefore, these results indicated that the marked increment in for sample 1 as compared to 3 is ascribed to the stronger light scattering, particularly at a red to near-infrared light region. It is thus postulated that both the light-scattering property and high dye-loading capacity from the integrated nanocrystalline composite electrodes resulted in the significant increase of IPCE as shown in Figure 5. In addition, it should be noted that the unaffected and effective electron diffusion coefficient in the double-layered TiO₂ is essential for the improved IPCE in sample 1.

Table 1: Photovoltaic characteristics of samples 1, 2, and 3 measured under AM1.5 illumination (100 mW cm⁻²). Each data represents the average of three cells with active area of 0.2 cm².

Sample
Thickness [μm]
[mA/cm²]
[V]
FF
[% ]
Adsorbed dye [μ mol cm⁻²]

1
8 + 6
18.40 0.05
0.73 0.02
0.69 0.01
9.25 0.05
1.163

2
8
13.04 0.03
0.73 0.02
0.67 0.01
6.38 0.05
1.012

3
10
14.86 0.03
0.70 0.02
0.68 0.01
7.07 0.05
1.171

Figure 4: Photocurrent and voltage curves for samples 1 and 2. Both measurements were performed under AM 1.5 G with the active area of 0.2 cm².

Figure 5: Incident monochromatic photon-to-current conversion efficiency (IPCE) as a function of excitation wavelength for samples 1 and 2.

4. Conclusions

We applied a facile colloidal template method for the preparation of spherical-cavity-based TiO₂/nanocrystalline TiO₂ double composite layers as a strong near-infrared light-scattering layer for N719-sensitized solar cells, which is particularly useful for the significant gain of photocurrents. The DSC fabricated by using double-layered electrodes composed of the scattering layer and the nanocrystalline TiO₂ layer produced a higher conversion efficiency of 9.25% versus 6.38% for the reference cell with a single TiO₂ electrode with the comparable thickness. The results obtained from our facile photon capture approach could open up new perspectives of exploiting low-cost and high-efficiency DSCs with a wide range of newly developed dye molecules and electrolytes.

Conflict of Interests

The authors declare that there is no conflict of interests.

Acknowledgments

The authors would like to acknowledge the National 863 Program (no. 2011AA050521) and 973 Program (no. 2006CB806200), National Science Foundation of China (nos. 20774103, 50625312, 60601027, 20421101, and U0634004), (No. 50973105), and the Koshiyama Research Grant in Japan for financial support.

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