Advances in Condensed Matter Physics

Volume 2014 (2014), Article ID 521493, 5 pages

http://dx.doi.org/10.1155/2014/521493

Research Article

Improved Composite Gel Electrolyte by Layered Vermiculite for Quasi-Solid-State Dye-Sensitized Solar Cells

Hongcai He,¹ Shuangshuang Ren,¹ Deting Kong,¹ and Ning Wang1,2

¹State Key Laboratory of Electronic Thin Films and Integrated Devices and School of Microelectronics and Solid-State Electronics, University of Electronic Science and Technology of China, Chengdu 610054, China

²Institute of Electronic and Information Engineering, University of Electronic Science and Technology of China, Dongguan 523808, China

Received 12 March 2014; Accepted 30 March 2014; Published 22 April 2014

Academic Editor: Ke Sun

Copyright © 2014 Hongcai He 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.

A composite quasisolid electrolyte is prepared by adding a layered vermiculite (VMT) into the iodide/triiodide electrolyte including 4-tert-butylpyridine, which obviously improves the photovoltaic properties of quasisolid dye-sensitized solar cells (DSSCs). When adding 6 wt% VMT, the maximum photovoltaic conversion efficiency of 3.89% is obtained, which reaches more than two times greater than that without VMT. This enhancement effect is primarily explained by studying the Nyquist spectra, dark currents, and photovoltaic conversion efficiency.

1. Introduction

Dye-sensitized solar cells (DSSCs) have attracted an ever-increasing attention since reported by O’Regan and Grätzel in 1991 [1] for its low-cost, environmental friendliness, and potential high conversion efficiency, which was considered to be a strong contender of the next-generation solar cells in the near future. Generally, a mainstream DSSC is composed of three main parts: a dye-adsorbed porous nanocrystalline TiO₂ film supported on a transparent conducting glass as the photoanode, an organic liquid electrolyte, essentially containing an iodide/triiodide redox couple, and a platinized transparent glass substrate as the counter electrode. These three layers are sandwiched together. Electrolytes play an important role in the DSSCs as the charge exchange medium. The organic liquid electrolyte was commonly used in traditional DSSCs, which is associated with problems such as hermetic sealing of the cell, solvent volatilization and leakage, bad long-term stability, decomposing dye, and corroding Pt electrode.

Recently, many efforts have been made to overcome the above problems of traditional DSSCs with liquid electrolytes, and solid-state and quasi-solid-state DSSCs have been intensely studied with various approaches. Some novel technologies and materials including p-type semiconductors [2], organic and inorganic holes conductors [3], and polymer gel electrolytes [4, 5] were used in new electrolytes to improve properties. Among them, polymer based quasi-solid-state electrolytes are a very good choice for its high ionic conductivity, long-term stability, good interfacial filling properties, and inhibiting leakage, which commonly have a polymer and ionic liquid electrolytes containing dispersed nanocomponents. Some ceramic nanoparticles such as SiO₂ [6], TiC [7] and TiN [8] were added into ionic liquids-based electrolytes for DSSCs, and an enhanced conversion efficiency was obtained. In our previous work [9, 10], some layered materials such as -zirconium phosphate and Mg-Al hydrotalcite were added into the iodide/triiodide ionic liquid to prepare quasi-solid-state electrolytes, which obviously improves the photovoltaic properties of quasisolid DSSCs. Vermiculite (VMT) is not only a layered mica-type silicate but is also with a large surface area and strong absorptive capacity and has often been studied for the preparation of composites [11, 12]. In this paper, a new composite gel polymer electrolyte was prepared by adding vermiculite (VMT) powder into iodide-based liquid electrolyte with the addition of 4-tert-butylpyridine (TBP), propylene carbonate (PC), and poly (ethylene oxide) (PEO-600,000). The electrochemical properties of the composite electrolyte were analyzed systematically by testing Nyquist diagram, and a typical DSSC was packaged with the new quasi-solid-state composite electrolyte to measure photovoltaic properties.

2. Experimental

2.1. Preparation of VMT and Composite Gel Polymer Electrolyte

The starting VMT was supplied by Bright Mining Co. (Shanghai, China). After VMT was ball-milled for 6 h in the solvent of deionized water, the ultrasonic irradiation method reported by Nguyen et al. [13] was used to prepare the layered vermiculite (VMT) powders.

Then, VMT powders with the contents of 0 wt%, 3 wt%, 6 wt%, 9 wt%, and 12 wt%, relative to the weight of TBP, were added to the iodide-based gel polymer electrolyte prepared according to [14], which contained 0.5 M LiI, 0.05 M I₂, 6 mL PC, 0.5 M TBP, 0.4 g PEO-600,000, and acetonitrile solvent. After stirring strongly for 72 h at 80°C, the composite gel polymer electrolytes including layered VMT were obtained.

2.2. Testing Device and Characterization Method

X-ray diffraction (XRD Rigaku D/max-RB) with CuKa radiation was used for phase analysis of the powders under 40 kV and 30 mA. Scanning electron microscopy (SEM, INSPECTF FEI, Netherlands) was used to observe the micrographs. Simple thin-layer cells were manufactured to measure AC impedance according to [15]. The cell was made up of two identical platinized TCO-coated glass substrates separated by Surlyn thermal packaging adhesive and filled with the composite electrolyte with VMT additives, as shown in Figure 1. The active area of the electrodes was about 0.16 cm² and the distance between the electrodes was about 25 μm. Electrochemical impedance spectra (EIS) were obtained by using CHI660c electrochemical analyzer (CH Instrument Co., ltd. China). Sinusoidal perturbations of 10 mV at frequencies from 0.01 Hz to 100 kHz with zero bias potential were applied on thin-layer cells with a two-electrode mode as shown in Figure 1. In order to study the photovoltaic properties of the DSSCs with the composite electrolytes containing VMT, quasisolid DSSCs were packaged according to the previous published procedures [9, 10] from dye-coated TiO₂ film photoanodes, counterelectrodes (500 nm thick, Pt), and composite gel polymer electrolytes containing VMT. Photovoltaic properties were measured at 100 mW cm⁻² light intensity under AM 1.5 irradiation of xenon lamp, while the dark current density is measured in dark. All measurements were carried out at room temperature.

Figure 1: Schematic diagram of the experimental thin-layer cell configuration employed for the electrochemical measurements.

3. Results and Discussion

3.1. Analysis of VMT Powders

Figure 2 shows a SEM micrograph of VMT powders, and the layered structure with a nanoscale layer thickness can be observed. X-ray diffraction patterns of the prepared VMT powder and composite electrolytes are shown in Figure 3. As shown in Figure 3(a), the prepared VMT powders are well-crystallized with the strongest diffraction peaks at 8.96°, indexed as (200) peak [13]. After 6 wt% VMT additive was mixed into iodine-based PEO electrolyte and coated on the photoanode thin film, the (200) peak was still detected in the obtained electrolyte membrane as shown in Figure 3(b).

Figure 2: SEM micrograph of VMT powder.

Figure 3: X-ray diffraction patterns of (a) VMT powder, (b) the composite electrolyte membrane with 6 wt% VMT, (c) the composite electrolyte membrane with 0 wt% VMT.

3.2. The Influence of VMT on the Conductivity

The Nyquist spectra of thin-layer cells with composite gel iodide-based electrolytes containing different contents of VMT are shown in Figure 4. The equivalent circuit is shown as the inset of Figure 4. Each curve is composed of two semicircles. The one in the high frequency region represents the charge transfer resistance () of Pt/electrolyte interface, and the other one in the low frequency region relates to the Warburg impedance () [8]. is the ohmic serial resistance and is the impedance of electrical double layer. Based on the equivalent circuit, the fitting data of the charge transfer resistance () and the ohmic serial resistance () were obtained. Then the ion conductivity of the electrolyte () can be obtained from the equation [4], where are are the active area of the electrodes (here  cm²) and the distance between electrodes (here  μm), respectively. The results for the values and values and corresponding values of iodide-based gel electrolytes with various contents of VMT are summarized in Table 1.

Table 1: The results for the and corresponding of the iodide-based gel electrolytes with various contents of VMT.

VMT (wt%)
()
()
(10⁻⁴ S cm⁻¹)

0
32.04
13.69
11.41

3
15.05
9.11
17.15

6
8.35
5.75
27.17

9
13.47
7.85
19.91

12
19.64
11.63
13.44

Figure 4: Nyquist diagram of thin-layer cells with various contents of VMT and the inset shows the equivalent circuit.

As shown in Figure 4 and Table 1, the values and the values of the cells decrease markedly and the corresponding values increase with adding VMT up to 6 wt%. Here, VMT as dispersed second phase insulating particles affected drastically the conductivities of composite iodide-based gel electrolytes. Quite a few works [16, 17] reported the effect of dispersed second phase particles on the ionic conduction. When adding the insulating phase in the ion-conductive phase, ionic conductivity will first increase and then decrease. Nan developed an improved and simple self-consistent effective-medium theory to explain the effect [18]. It has now become widely accepted that the enhancement effect of conductivity is related to creating highly conductive paths along the interfaces between the electrolyte matrix and the second phase grains [18]. The highly conductive paths can be an interfacial layer with high concentrations of defects, a space charge layer, and/or an absorbed water layer. VMT has a layered structure with a large surface area, which means there is enough interface to create conductive paths. When the content of VMT is 6 wt%, the minimum value of 8.35 Ω and the minimum value of 5.75 Ω are obtained, corresponding with the maximum value of 27.17 10⁻⁴ S cm⁻¹. While the content of VMT is over 6 wt%, the inert second phase particles directly contact each other to form continuum percolation net clusters, which tends to limit ion movement and decrease the conductivity [17, 18], and, as a result, the values and the value increase and the values decrease markedly.

3.3. The Influence of VMT on the Photovoltaic Conversion Efficiency

Figure 5(a) is the curves of thin-layer cells with various VMT contents. The results for short-circuit current density (), open circuit potential (), fill factor (FF), and conversion efficiency () of the DSSCs with different additions of VMT are summarized in Table 2. The DSSCs with the electrolytes adding VMT show a higher open circuit potential () and significantly higher short current density () than that without adding VMT. and increase first and then decrease with the increase of VMT contents. In order to study the influence of electrolytes with adding various contents of VMT on the above photoelectric properties, the dark current density-voltage curves of the DSSCs with various contents of VMT are shown in Figure 5(b). It can be easily found that the dark current density decreases when adding the VMT. As the content of VMT increases to 6 wt%, the dark current density of the DSSC is suppressed to a minimum and increases quickly as the content of VMT further increases over 6 wt% to 12 wt%.

Table 2: The photovoltaic parameters of the DSSCs with various contents of VMT.

VMT (wt%)
(mA cm⁻²)
(V)
FF
(%)

0
5.08
0.62
0.54
1.70

3
9.07
0.64
0.53
3.07

6
9.77
0.67
0.59
3.89

9
8.53
0.66
0.55
3.10

12
7.15
0.64
0.53
2.43

(a)

(b)

Figure 5: The curves of DSSCs with composite electrolytes containing various contents of VMT (a) under simulated AM 1.5 solar spectrum irradiation at 100 mW cm⁻²; (b) in the dark.

The change in both and of the DSSCs is related to the dark current density. The enhanced is due to the suppression of the dark current in the TiO₂/electrolyte interface. The fact that the onset of the dark current of DSSCs occurs at the higher forward bias indicates the lower reduction rate () [9, 19]. The decrease of reduction rate will lead to an increase of according to the following equation [19]:

where , , and are the flux of charge originating from sensitized injection related to the electron back transfer rate, the concentration of electrons at the TiO₂ surface, and the rate constants for reduction, respectively. As shown in Figure 5(b), the onset of the dark current of DSSCs occurs at 227, 335, 378, 325, and 319 mV with various electrolytes adding 0 wt%, 3 wt%, 6 wt%, 9 wt%, and 12 wt% of VMT, respectively. The higher onset voltage value of the dark current of DSSCs with adding VMT than that without adding VMT reveals that VMT can efficiently suppress the dark reaction to obtain higher . On the other hand, the of DSSCs is also associated with the dark current, which can be given by the equation , where and are the electron injection current density and the recombination current density, respectively [20]. The electron injection current density should be constant since all the DSSCs have the same electrodes and experimental conditions. The recombination current mainly manifests as the dark current, so the recombination current density has similar variation trend with the dark current density [21]. Consequently increases with the decrease of the dark current density. As a consequence, proper addition of VMT can improve both and of the DSSC, and the best ratio is about 6 wt% of VMT. When the content of VMT is 6 wt%, the conversion efficiency () is up to the maximum of 3.89%, which is more than two times greater than that without adding VMT. While the content of VMT is over 6 wt%, the conversion efficiency () decreases quickly.

4. Conclusions

In summary, we prepared a quasi-solid-state composite electrolyte by adding layered vermiculite (VMT) powder into the iodide-based electrolyte including PC, TBP, and PEO-600,000. Electrochemical analysis was done on the DSSCs with various electrolytes adding different contents of VMT. The results showed that VMT as a dispersed second phase insulating particles affected drastically the conductivities of composite electrolytes. The reduction of the dark current density with adding VMT indicated that the and increased with the addition of appropriate amount of VMT, compared to DSSCs without VMT. When the content of VMT reached 6 wt%, the conversion efficiency () was maximized to 3.89%, which was more than two times greater than that without addition of the VMT.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgments

This work was supported by Natural Science Foundation of China (51272035, 51272037, and 51362026), International Cooperation MOST-JST Program Fund (no. 2010DFA61410), The Project of International Cooperation of the Ministry of Science and Technology of China (no. 2011DFA50530), and Scientific Research Project of Guangdong (no. 2012B091000015).

References

B. O'Regan and M. Grätzel, “A low-cost, high-efficiency solar cell based on dye-sensitized colloidal TiO₂ films,” Nature, vol. 353, no. 6346, pp. 737–740, 1991.

K. Tennakone, G. K. R. Senadeera, D. B. R. A. De Silva, and I. R. M. Kottegoda, “Highly stable dye-sensitized solid-state solar cell with the semiconductor 4CuBr 3S(C₄H₉)₂ as the hole collector,” Applied Physics Letters, vol. 77, no. 15, pp. 2367–2369, 2000.

C. S. Karthikeyan, H. Wietasch, and M. Thelakkat, “Highly efficient solid-state dye-sensitized TiO₂ solar cells using donor-antenna dyes capable of multistep charge-transfer cascades,” Advanced Materials, vol. 19, no. 8, pp. 1091–1095, 2007.

X. Chen, Q. Li, J. Zhao et al., “Ionic liquid-tethered nanoparticle/poly(ionic liquid) electrolytes for quasi-solid-state dye-sensitized solar cells,” Journal of Power Sources, vol. 207, pp. 216–221, 2012.

P. Wang, S. M. Zakeeruddin, J. E. Moser, M. K. Nazeeruddin, T. Sekiguchi, and M. Grätzel, “A stable quasi-solid-state dye-sensitized solar cell with an amphiphilic ruthenium sensitizer and polymer gel electrolyte,” Nature Materials, vol. 2, no. 6, pp. 402–407, 2003.

K.-M. Lee, P.-Y. Chen, C.-P. Lee, and K.-C. Ho, “Binary room-temperature ionic liquids based electrolytes solidified with SiO₂ nanoparticles for dye-sensitized solar cells,” Journal of Power Sources, vol. 190, no. 2, pp. 573–577, 2009.

C.-P. Lee, K.-M. Lee, P.-Y. Chen, and K.-C. Ho, “On the addition of conducting ceramic nanoparticles in solvent-free ionic liquid electrolyte for dye-sensitized solar cells,” Solar Energy Materials and Solar Cells, vol. 93, no. 8, pp. 1411–1416, 2009.

C.-P. Lee, L.-Y. Lin, R. Vittal, and K.-C. Ho, “Favorable effects of titanium nitride or its thermally treated version in a gel electrolyte for a quasi-solid-state dye-sensitized solar cell,” Journal of Power Sources, vol. 196, no. 3, pp. 1665–1670, 2011.

N. Wang, H. Lin, J. Li, and X. Li, “Improved quasi-solid dye-sensitized solar cells by composite ionic liquid electrolyte including layered α -zirconium phosphate,” Applied Physics Letters, vol. 89, no. 19, Article ID 194104, 2006.

H. He, J. Zhu, N. Wang, F. Luo, and K. Yang, “Composite gel polymer electrolytes containing layered Mg-Al hydrotalcite for quasi-solid dye-sensitized solar cells,” Journal of the Electrochemical Society, vol. 161, pp. H17–H20, 2014.

M. V. Smalley, H. L. M. Hatharasinghe, I. Osborne, J. Swenson, and S. M. King, “Bridging flocculation in vermiculite—PEO mixtures,” Langmuir, vol. 17, no. 13, pp. 3800–3812, 2001.

L. Zang, J. Luo, J. Guo, H. Liu, and J. Ru, “Preparation and characterization of poly(ethylene glycol)/organo- vermiculite nanocomposite polymer electrolytes,” Polymer Bulletin, vol. 65, no. 7, pp. 669–680, 2010.

A. N. Nguyen, L. Reinert, J. M. Lévêque et al., “Preparation and characterization of micron and submicron-sized vermiculite powders by ultrasonic irradiation,” Applied Clay Science, vol. 72, pp. 9–17, 2013.

Y. Ren, Z. Zhang, S. Fang, M. Yang, and S. Cai, “Application of PEO based gel network polymer electrolytes in dye-sensitized photoelectrochemical cells,” Solar Energy Materials and Solar Cells, vol. 71, no. 2, pp. 253–259, 2002.

N. Papageorgiou, W. F. Maier, and M. Grätzel, “An iodine/triiodide reduction electrocatalyst for aqueous and organic media,” Journal of the Electrochemical Society, vol. 144, no. 3, pp. 876–884, 1997.

C. C. Liang, “Conduction characteristics of the lithium iodide—aluminum oxide solid electrolytes,” Journal of the Electrochemical Society, vol. 120, no. 10, pp. 1289–1292, 1973.

C.-W. Nan, L. Fan, Y. Lin, and Q. Cai, “Enhanced ionic conductivity of polymer electrolytes containing nanocomposite SiO₂ particles,” Physical Review Letters, vol. 91, no. 26, pp. 2661041–2661044, 2003.

C.-W. Nan, “Physics of inhomogeneous inorganic materials,” Progress in Materials Science, vol. 37, no. 1, pp. 1–116, 1993.

M. K. Nazeeruddin, A. Kay, I. Rodicio et al., “Conversion of light to electricity by cis-X2bis(2,2′-bipyridyl-4,4′-dicarboxylate)ruthenium(II) charge-transfer sensitizers (X = Cl-, Br-, I-, CN-, and SCN-) on nanocrystalline TiO₂ electrodes,” Journal of the American Chemical Society, vol. 115, no. 14, pp. 6382–6390, 1993.

L. Y. Chen and Y. T. Yin, “The influence of length of one-dimensional photoanode on the performance of dye-sensitized solar cells,” Journal of Materials Chemistry, vol. 22, no. 47, pp. 24591–24596, 2012.

K. Guo, M. Li, X. Fang et al., “Preparation and enhanced properties of dye-sensitized solar cells by surface plasmon resonance of Ag nanoparticles in nanocomposite photoanode,” Journal of Power Sources, vol. 230, pp. 155–160, 2013.