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Advances in OptoElectronics
Volume 2011 (2011), Article ID 357974, 7 pages
Quasi Solid-State Dye-Sensitized Solar Cell Incorporating Highly Conducting Polythiophene-Coated Carbon Nanotube Composites in Ionic Liquid
1Center of Excellence for Research in Engineering Materials (CEREM), College of Engineering, King Saud University, Riyadh 11421, Saudi Arabia
2Photovoltaic Materials Unit, National Institute for Materials Science (NIMS), 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan
Received 30 April 2011; Accepted 13 June 2011
Academic Editor: Ahmed El-Shafei
Copyright © 2011 Mohammad Rezaul Karim 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.
Conducting polythiophene (PTh) composites with the host filler multiwalled carbon nanotube (MWNT) have been used, for the first time, in the dye-sensitized solar cells (DSCs). A quasi solid-state DSCs with the hybrid MWNT-PTh composites, an ionic liquid of 1-methyl-3-propyl imidazolium iodide (PMII), was placed between the dye-sensitized porous TiO2 and the Pt counter electrode without adding iodine and higher cell efficiency (4.76%) was achieved, as compared to that containing bare PMII (0.29%). The MWNT-PTh nanoparticles are exploited as the extended electron transfer materials and serve simultaneously as catalyst for the electrochemical reduction of .
Dye-sensitized solar cells (DSCs) have attracted significant attention as promising solar-to-electricity power conversion devices because of their higher energy conversion and potential for low-cost production [1–6]. In general, DSCs comprise an electrode consisting of nanocrystalline titanium dioxide (TiO2) films modified with a dye, a platinum counterelectrode, and an electrolyte solution in between the electrodes. Photoexcitation of the dye results in the injection of an electron into the conduction band of the oxide. The original state of the dye is subsequently restored by electron donation from a redox system, such as the iodide/triiodide (I−/I3 −) couple. At the present, DSCs are mainly constructed by using liquid electrolyte as a charge transport material. The charge transport in these liquid electrolytes is typically achieved by using I−/I3 − redox reaction in electrolyte solution. Therefore, long-term durability of DSCs is limited by leakage and the volatilization of organic solvent-based electrolytes. Numerous investigations have been conferred to overcome this drawback, replacing the liquid electrolyte by organic and inorganic hole transport materials [7–9], polymer and gel electrolytes [10–14], and nanocomposite ionic liquid (IL) electrolytes [15–20] resulting in solid-state and quasi solid-state DSCs. Imperfect pour filling of the dye-coated nanocrystalline TiO2 film with organic and inorganic hole transport materials results in a poor device efficiency. Moreover, the ionic conductivity for the majority of the amorphous polymer electrolytes is too low (<10−5 S cm−1), limiting the device efficiency. Although nanocomposite IL electrolyte can reduce leakages, it is not satisfactory, because of the high concentration of corrosive and volatile iodine present in the electrolyte. The introduction of I2 into the electrolytes could increase the conductivity of the electrolyte via a Grotthuss-type charge carrier exchange transfer mechanism. However, the increasing content of I2 (or I3 −) leads to enhanced light absorption even in the visible range by the electrolyte. The increased absorption of visible light by the electrolyte, the enhanced dark current, and the reduced ionic conductivity of the electrolyte contribute to the performance variation of the corresponding DSCs with increasing I2 concentration.
Conducting polymer-coated carbon nanotube composites are extremely good conducting hybrid materials, which are often used in organic field effect transistor, solar cells, sensors, electrochromic devices, and light emitting diodes [21–24]. Lee and coworkers reported iodine-free quasi solid-state DSCs, containing a conducting polymer loaded carbon black and an ionic liquid, which exhibited a power conversion efficiency of 5.8% . Recently, Lee et al. further reported an efficient solid-state DSC using a hybrid carbon nanotubes-binary ionic liquid containing1-ethyl-3-methylimidazolium iodide (EMII) and 1-methyl-3-propylimidazolium iodine (PMII), without the addition of iodine and TBP . Besides, Wang et al. and Ikeda et al. have reported separately a solid-state electrolyte without the incorporation of volatile iodine and achieved high device efficiency [27, 28].
In our earlier work, we reported highly conducting cable-like PTh-MWNT composites, composed of conducting polythiophene (PTh) with the host filler multiwalled carbon nanotube (MWNT), synthesized by the gamma-radiation-induced in situ chemical polymerization method . In this study, core-shell MWNT-PTh composites were added to ionic liquid to form the extended electron transfer surface (Scheme 1) from the counterelectrode’s surface to the bulk electrolyte, in order to facilitate electron transfer and, thereby, decrease the dark current from the working electrode to the electrolyte. For the first time, MWNT-PTh composites have been used in DSSC, and the effect of MWNT-PTh composites addition in the solvent-free ionic liquid electrolyte without the incorporation of iodine was studied.
The following chemicals were purchased and used without further purification: iodine (I2, from Merck), 1-methyl-3-propyl-imidazoliumiodide (MPII, from Merck), tert-butyl alcohol (Fluka), acetonitrile (ACN, 99.99%, Aldrich), anhydrous iron (III) chloride (FeCl3, Aldrich), and chloroform (CHCl3, Aldrich). Thiophene monomer (99+%, Aldrich) was distilled under a reduced pressure and kept below 0°C prior to use. MWNT (>95 vol. grade, produced by the CVD method; diameter: 10~20 nm, length: 10~50 μm) was supplied by Iljin Nanotech Co., Ltd., Republic of Korea.
2.2. Composite Electrolyte
The conducting MWNT-PTh hybrid composites were synthesized as per our reported work . The instruments used for the characterization of MWNT-PTh hybrid composites included a field-emission scanning electron microscope (FE-SEM) (Hitachi Model S-4300) and a transmission electron microscope (TEM) (Philips model CM 200) with an Acc. Voltage of 200 kv. The room-temperature conductivity of the pressed pellets was measured by the four-point probe method using a Jandel engineering instrument, Model CMT-SR1060N. The composite electrolyte was prepared by mixing the solid powder of MWNT-PTh, PMII, and ACN in a weight ratio of 1 : 7 : 7. ACN was added to the composite to improve the mixing, and was removed on a hot plate at a temperature of 90°C.
2.3. Fabrication of Dye-Sensitized Solar Cell
Nanocrystalline TiO2 photoelectrodes of 15 μm thickness (area: 0.25 cm2) were prepared on conducting glass using a variation of a previously reported method . Fluorine-doped tin oxide-coated glass electrodes (Nippon Sheet Glass Co., Japan) with a sheet resistance of 8–10 ohm−2 and an optical transmission of greater than 80% in the visible range were used. Anatase TiO2 colloid pastes (particle size ~25 nm and ~400 nm) were obtained from commercial sources (Solaronix). The nanocrystalline TiO2 thin films of approximately 15 μm thickness were deposited onto the conducting glass by screen printing. The film was sintered at 500°C for 1 h. The film thickness was measured with a Surfcom 1400 A surface profiler (Tokyo Seimitsu Co. Ltd.). The electrodes were impregnated with a 0.05 M titanium tetrachloride solution and sintered at 500°C. A dye solution of 3 × 10−4 M N719 was prepared in 1 : 1 acetonitrile and tert-butyl alcohol solvents. Deoxycholic acid (20 mM) was added to the dye solution as a coadsorbent to prevent aggregation of the dye molecules [31, 32]. The electrodes were immersed in the N719 solution and then kept at 25°C for 20 h to adsorb the dye onto the TiO2 surface. Photovoltaic measurements were performed in a two-electrode sandwich cell configuration. The dye-deposited TiO2 film and a platinum-coated conducting glass were used as the working electrode and the counterelectrode, respectively. A 30 μm thick surlyn spacer was put on the dye-deposited TiO2 electrode and attached by heating. The MWNT-PTh/MPII hybrid composite electrolyte was then put onto the dye-sensitized TiO2 film at 85°C to ensure that the PMII can penetrate well into the porous structure and remove the residual ACN. The dye-deposited TiO2 electrode with the MWNT-PTh/MPII hybrid composite electrolytes was assembled with a platinum-coated conducting glass electrode and sealed by heating the polymer frame. The electrolytes used for liquid cell were composed of 0.6 M dimethylpropyl-imidazolium iodide (DMPII), 0.05 M I2, and 0.1 M LiI in acetonitrile.
2.4. Photovoltaic Characterization
The working electrode was illuminated through a conducting glass. The current-voltage characteristics were measured using a solar simulator (AM-1.5, 100 mW/cm2, WXS-155S-10: Wacom Denso Co., Japan). Monochromatic incident photon-to-current conversion efficiency (IPCE) for the solar cell, plotted as a function of excitation wavelength, was recorded on a CEP-2000 system (Bunkoh-Keiki Co., Ltd.). Incident photon-to-current conversion efficiency (IPCE) at each incident wavelength was calculated from (1), where is the photocurrent density at short circuit in mA cm−2 under monochromatic irradiation, is the elementary charge, is the wavelength of incident radiation in nm, and is the incident radiative flux in W m−2:
3. Results and Discussion
Room temperature ionic liquids have several qualities as compared with other choices since they have negligible volatility, high thermal stability, a wide electrochemical potential window, and satisfactory ionic conductivity [33, 34]. Ionic liquids have limited ion diffusion because of its high viscosity. The conductivity of ionic liquid electrolytes is further improved by increasing iodine concentration resulting in a polyiodide formation thus facilitating electron-exchange-type conductivity . Increasing of iodine concentration is, however, limited by strong visible light absorption by iodine itself. Therefore, iodide ionic liquids in combination with moderately high iodine concentration only make a satisfactory electrolyte for DSCs. Moreover, it was reported that the carbon material in the iodine-free composite electrolyte serves simultaneously as a charge transporter in the electrolyte and as a catalyst for electrochemical reduction of I3 − ions . The iodide anion-based IL can provide sufficient I− for the regeneration of oxidized dye under illumination; I− in turn oxidizes to I3 −, which can be reduced back to I− at the carbon material.
A main component of DSCs is the electrolyte that fills the space between the dye-coated porous nanocrystalline TiO2 electrode and the counterelectrode. In the vast majority of cases the electrolyte contains I−/I3 − redox couple. In general, iodide salt and iodine are the source of the I−/I3 − redox couple. In the electrolyte, I2 exists in the form of polyiodides such as I3 − or I5 − (2). Photoexcitation of the dye results in the injection of an electron into the conduction band of the TiO2. The oxidized state of the dye (dye+) should be regenerated efficiently by electron donation from I− (3). The efficient regeneration of oxidized dye is crucial for obtaining good electron collection yields and a high cycle life of the sensitizer. Meanwhile, the electrons accumulated at the counterelectrode by the external circuit will lead to concentration over potentials for the electrolyte at the counterelectrode and loss of energy of the DSCs if the electrons are not transferred by I3 − efficiently (4). Apart from recapture by the oxidized dye, the electrons can be lost to the electrolyte by reaction with the I3 − (5). Therefore an efficient transport of iodide and triiodide in the electrolyte is necessary for good performance of the DSCs. Meanwhile, the increase of the I3 − concentration in the electrolyte results in an increasing dark current of the DSCs and thus decreases the device performance:
Conducting polymer-coated carbon nanotubes are notable materials, which are being widely studied because of their extraordinary electronic and mechanical properties. Considering these aspects, incombustible and nonvolatile PMII and MWNT-PTh composites, were incorporated into DSCs for this study (Scheme 1). The presence of redox-active PMII ionic liquid fills the nanoporous TiO2/dye interface, where no space is available for MWNT-PTh composites to occupy. It is expected that this IL would allow perfect contact at the interface between the dye-coated porous TiO2 and the conducting polymer-coated carbon material , that is, MWNT-PTh composites.
A typical morphology of MWNT-PTh composites synthesized by the radiolysis polymerization method was investigated using scanning electron microscopes (Figure 1). In Figure 1(a), the FE-SEM image shows a uniform view of the MWNT-PTh composites. The tubular morphology of the MWNT-PTh composites was also imaged by the TEM, as shown in Figure 1(b). Structural characterizations showed that there was clear indication of interfacial entrapment between the PTh and MWNT; the conducting polymer is coated on the surface of the carbon nanotube. Here, the tubular inner part (core) is mainly the compound of MWNT and the outer coated surface (shell) is conducting polythiophene with variable thicknesses (20–50 nm diameters), and their external surfaces are not smooth.
Figure 2 shows the energy dispersive spectroscopy (EDS) analysis of MWNT-PTh composites (data are given in the table). The atomic percents of the C and S are 58.78 and 11.75, respectively, for MWNT-PTh composites which reveal that carbon nanotube and polythiophene are both present in the sample. In general, electrical conductivity may be taken as a function of the conjugation length of the polymer and the amount of active dopant present in the polymer, as the number of charge carriers depends upon the extent of the dopant concentration, provided that other factors remain unchanged. A powder sample of 0.02 g was loaded and pressed into a pellet 1.2 cm in diameter and a pressure of 170 atm by a manual hydraulic press for 10 min. Then, the electrical conductivity of the pellets was measured by a standard four-point probe method, connected to a Keithley voltmeter-constant current source system. The conductivity of the resulting MWNT-PTh composites at room temperature is 3.2 S cm−1, which is higher than that of the pristine PTh (~1.1 × 10−4 S cm−1), which is synthesized without MWNT, under the same conditions. The combination of PTh with MWNT has effectively increased the conductivity four orders of magnitude for the MWNT-PTh composites compared with the counterpart bulk PTh powders. A lower resistance is expected for MWNT-PTh/PMII composites electrolyte compared to that of bare PMII.
The photovoltaic performances of the DSCs under AM 1.5 G simulated solar light at a light intensity of 100 mW cm−2 using MWNT-PTh/PMII composite electrolyte and using bare PMII as electrolyte are shown in Table 1. The cell efficiency of MWNT-PTh/PMII device is 4.76%, which is remarkably higher than that of bare PMII device (0.29%). The low device efficiency of bare PMII device is due to significant decrease in both and FF. The presence of PTh-MWNT facilitates electron transfer from counterelectrode to I3 − ions in MWNT-PTh/PMII composite device. Recently, Lee et al. reported, based on electrochemical impedance spectroscopy (EIS) analysis, that the presence of carbon materials in IL facilitates electron transfer from counterelectrode to I3 −, which enables the I−/I3 − redox couple to work more efficiently than they would in the absence of carbon materials . An analogous explanation is also assumed for the MWNT-PTh/PMII composite electrolyte systems as well.
Figure 3 shows a photocurrent density-voltage curve of a sealed solar cell based on MWNT-PTh/PMII under AM 1.5 G simulated solar light at a light intensity of 100 mW cm−2. The MWNT-PTh/PMII electrolyte containing solar cell showed a photocurrent density of 10.2 mA cm−2, an open-circuit potential of 0.73 V, and a fill factor of 0.64, corresponding to an overall conversion efficiency (η) of 4.76%. In the same experimental condition, liquid electrolyte device shows an overall conversion efficiency (η) of 7.86% with a high photocurrent density of 15.4 mA cm−2 (Table 1). Figure 4 shows the monochromatic incident photon to current conversion efficiency (IPCE) for DSCs based on MWNT-PTh/PMII composite and liquid electrolytes. Liquid-electrolyte-based device shows the maximum IPCE of 74% at 540 nm, while the MWNT-PTh/PMII device shows only 59% IPCE at 540 nm. Inefficient charge transport properties in the composite electrolyte may be responsible for the low conversion efficiency in the MWNT-PTh/PMII-electrolyte-based device. Further study will target the development of a high-performance quasi solid-state solar cell through improvement of charge transport properties in the composite electrolyte and also the catalytic activity of the electrolyte for electrochemical reduction of I3 − ions.
A 4.76% of light-to-electricity conversion efficiency of the quasi solid-state DSCs is obtained using hybrid MWNT-PTh/PMII composites electrolyte without the addition of iodine under the radiation of 100 mW cm−2 (AM1.5 full sunlight). The cell efficiency of the quasi solid-state DSCs incorporating highly conducting MWNT-PTh composite is one order higher than that of bare PMII device (0.29%). It is assumed that the hybrid MWNT-PTh composite plays a key role in both charge transportation in the composite electrolyte and the catalytic activities for electrochemical reduction of I3 −.
The authors gratefully acknowledge the financial support from NPST program by King Saud University of project no. 10-NAN1021-02.
- 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.
- A. Hagfeld and M. Grätzel, “Light-induced redox reactions in nanocrystalline systems,” Chemical Reviews, vol. 95, no. 1, pp. 49–68, 1995.
- M. Grätzel, “Conversion of sunlight to electric power by nanocrystalline dye-sensitized solar cells,” Journal of Photochemistry and Photobiology A, vol. 164, no. 1–3, pp. 3–14, 2004.
- A. Hagfeldt and M. Grätzel, “Molecular photovoltaics,” Accounts of Chemical Research, vol. 33, no. 5, pp. 269–277, 2000.
- 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.
- K. Hara, H. Sugihara, Y. Tachibana et al., “Dye-sensitized nanocrystalline TiO2 solar cells based on ruthenium(II) phenanthroline complex photosensitizers,” Langmuir, vol. 17, no. 19, pp. 5992–5999, 2001.
- J. Bandara and H. Weerasinghe, “Solid-state dye-sensitized solar cell with p-type NiO as a hole collector,” Solar Energy Materials and Solar Cells, vol. 85, no. 3, pp. 385–390, 2005.
- G. K. R. Senadeera, T. Kitamura, Y. Wada, and S. Yanagida, “Enhanced photoresponses of polypyrrole on surface modified TiO2 with self-assembled monolayers,” Journal of Photochemistry and Photobiology A, vol. 184, no. 1-2, pp. 234–239, 2006.
- J. E. Kroeze, N. Hirata, L. Schmidt-Mende et al., “Parameters influencing charge separation in solid-state dye-sensitized solar cells using novel hole conductors,” Advanced Functional Materials, vol. 16, no. 14, pp. 1832–1838, 2006.
- T. Kato, A. Okazaki, and S. Hayase, “Latent gel electrolyte precursors for quasi-solid dye sensitized solar cells the comparison of nano-particle cross-linkers with polymer cross-linkers,” Journal of Photochemistry and Photobiology A, vol. 179, no. 1-2, pp. 42–48, 2006.
- J. N. Freitas, C. Longo, A. F. Nogueira, and M.-A. de Paoli, “Solar module using dye-sensitized solar cells with a polymer electrolyte,” Solar Energy Materials and Solar Cells, vol. 92, no. 9, pp. 1110–1114, 2008.
- J. Wu, Z. Lan, J. Lin et al., “A novel thermosetting gel electrolyte for stable quasi-solid-state dye-sensitized solar cells,” Advanced Materials, vol. 19, no. 22, pp. 4006–4011, 2007.
- J. N. Freitas, A. F. Nogueira, and M.-A. de Paoli, “New insights into dye-sensitized solar cells with polymer electrolytes,” Journal of Materials Chemistry, vol. 19, no. 30, pp. 5279–5294, 2009.
- B. I. Ito, J. N. De Freitas, M. A. De Paoli, and A. F. Nogueira, “Application of a composite polymer electrolyte based on montmorillonite in dye-sensitized solar cells,” Journal of the Brazilian Chemical Society, vol. 19, no. 4, pp. 688–696, 2008.
- P. Wang, S. M. Zakeeruddin, P. Comte, I. Exnar, and M. Grätzel, “Gelation of ionic liquid-based electrolytes with silica nanoparticles for quasi-solid-state dye-sensitized solar cells,” Journal of the American Chemical Society, vol. 125, no. 5, pp. 1166–1167, 2003.
- H. Usui, H. Matsui, N. Tanabe, and S. Yanagida, “Improved dye-sensitized solar cells using ionic nanocomposite gel electrolytes,” Journal of Photochemistry and Photobiology A, vol. 164, no. 1–3, pp. 97–101, 2004.
- T. Katakabe, R. Kawano, and M. Watanabe, “Acceleration of redox diffusion and charge-transfer rates in an ionic liquid with nanoparticle addition,” Electrochemical and Solid-State Letters, vol. 10, no. 6, pp. F23–F25, 2007.
- 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.
- Z. Chen, H. Yang, X. Li, F. Li, T. Yi, and C. Huang, “Thermostable succinonitrile-based gel electrolyte for efficient, long-life dye-sensitized solar cells,” Journal of Materials Chemistry, vol. 17, no. 16, pp. 1602–1607, 2007.
- W. U. Huynh, J. J. Dittmer, and A. P. Alivisatos, “Hybrid nanorod-polymer solar cells,” Science, vol. 295, no. 5564, pp. 2425–2427, 2002.
- M. R. Karim, C. J. Lee, and M. S. Lee, “Synthesis and characterization of conducting polythiophene/carbon nanotubes composites,” Journal of Polymer Science A, vol. 44, no. 18, pp. 5283–5290, 2006.
- M. R. Karim, C. J. Lee, Y.-T. Park, and M. S. Lee, “SWNTs coated by conducting polyaniline: synthesis and modified properties,” Synthetic Metals, vol. 151, no. 2, pp. 131–135, 2005.
- M. Fu, Y. Zhu, R. Tan, and G. Shi, “Aligned polythiophene micro- and nanotubules,” Advanced Materials, vol. 13, no. 24, pp. 1874–1877, 2001.
- C.-P. Lee, P. Y. Chen, R. Vittal, and K.-C. Ho, “Iodine-free high efficient quasi solid-state dye-sensitized solar cell containing ionic liquid and polyaniline-loaded carbon black,” Journal of Materials Chemistry, vol. 20, no. 12, pp. 2356–2361, 2010.
- C.-P. Lee, L.-Y. Lin, P.-Y. Chen, R. Vittal, and K.-C. Ho, “All-solid-state dye-sensitized solar cells incorporating SWCNTs and crystal growth inhibitor,” Journal of Materials Chemistry, vol. 20, no. 18, pp. 3619–3625, 2010.
- H. Wang, H. Li, B. Xue, Z. Wang, Q. Meng, and L. Chen, “Solid-state composite electrolyte Lil/3-hydroxypropionitrile/SiO2 for dye-sensitized solar cells,” Journal of the American Chemical Society, vol. 127, no. 17, pp. 6394–6401, 2005.
- N. Ikeda, K. Teshima, and T. Miyasaka, “Conductive polymer-carbon-imidazolium composite: a simple means for constructing solid-state dye-sensitized solar cells,” Chemical Communications, no. 16, pp. 1733–1735, 2006.
- M. R. Karim, J. H. Yeum, M. S. Lee, and K. T. Lim, “Synthesis of conducting polythiophene composites with multi-walled carbon nanotube by the γ-radiolysis polymerization method,” Materials Chemistry and Physics, vol. 112, no. 3, pp. 779–782, 2008.
- M. K. Nazeeruddin, P. Péchy, T. Renouard et al., “Engineering of efficient panchromatic sensitizers for nanocrystalline TiO2-based solar cells,” Journal of the American Chemical Society, vol. 123, no. 8, pp. 1613–1624, 2001.
- M. Ikeda, N. Koide, L. Han, A. Sasahara, and H. Onishi, “Scanning tunneling microscopy study of black dye and deoxycholic acid adsorbed on a rutile TiO2(110),” Langmuir, vol. 24, no. 15, pp. 8056–8060, 2008.
- Z. S. Wang, Y. Cui, Y. Dan-oh, C. Kasada, A. Shinpo, and K. Hara, “Thiophene-functionalized coumarin dye for efficient dye-sensitized solar cells: electron lifetime improved by coadsorption of deoxycholic acid,” Journal of Physical Chemistry C, vol. 111, no. 19, pp. 7224–7230, 2007.
- N. Papageorgiou, Y. Athanassov, M. Armand et al., “The performance and stability of ambient temperature molten salts for solar cell applications,” Journal of the Electrochemical Society, vol. 143, no. 10, pp. 3099–3108, 1996.
- P. Wang, S. M. Zakeeruddin, J. E. Moser, R. H. Baker, and M. Grätzel, “A solvent-free, SeCN-/based ionic liquid electrolyte for high-efficiency dye-sensitized nanocrystalline solar cells,” Journal of the American Chemical Society, vol. 126, no. 23, pp. 7164–7165, 2004.
- R. Kawano, H. Matsui, C. Matsuyama et al., “High performance dye-sensitized solar cells using ionic liquids as their electrolytes,” Journal of Photochemistry and Photobiology A, vol. 164, no. 1–3, pp. 87–92, 2004.