Advanced
Effect of SiO2/ITO Film on Energy Conversion Efficiency of Dye-sensitized Solar Cells
Effect of SiO2/ITO Film on Energy Conversion Efficiency of Dye-sensitized Solar Cells
Transactions on Electrical and Electronic Materials. 2015. Dec, 16(6): 303-307
Copyright © 2015, The Korean Institute of Electrical and Electronic Material Engineers
This is an open-access article distributed under the terms of the Creative Commons Attribution Non-Commercial License (http://creativecommons.org/licenses/by-nc/3.0) which permits unrestricted noncommercial use, distribution, and reproduction in any medium, provided the original work is properly cited.
  • Received : September 09, 2015
  • Accepted : October 10, 2015
  • Published : December 25, 2015
Download
PDF
e-PUB
PubReader
PPT
Export by style
Share
Article
Author
Metrics
Cited by
TagCloud
About the Authors
Jong-Su Woo
Gun-Eik Jang
gejang@chungbuk.ac.kr
Abstract
Multilayered films of ITO (In 2 O 3 :SnO 2 = 9:1)/SiO 2 were deposited on soda-lime glass by RF/DC magnetron sputtering at 500℃ to improve the energy conversion efficiency of dye-sensitized solar cells (DSSCs). The light absorption of the dye was improved by decrease in light reflectance from the surface of the DSSCs by using an ITO film. In order to estimate the optical characteristics and compare them with experimental results, a simulation program named EMP (essential macleod program) was used. EMP results revealed that the multilayered thin films showed high transmittance (approximate average transmittance of 79%) by adjusting the SiO 2 layer thickness. XRD results revealed that the ITO and TiO 2 films exhibited a crystalline phase with (400) and (101) preferred orientations at 2 θ = 26.24° and 35.18°, respectively. The photocurrent-voltage (I-V) characteristics of the DSSCs were measured under AM 1.5 and 100 mW/cm 2 (1 sun) by using a solar simulator. The DSSC fabricated on the ITO film with a 0.1-nm-thick SiO 2 film showed a Voc of 0.697 V, J sc of 10.596 mA/cm 2 , FF of 66.423, and calculated power conversion efficiency (η AM1.5 ) of 5.259%, which was the maximum value observed in this study.
Keywords
1. INTRODUCTION
Dye-sensitized solar cells (DSSCs) have attracted increasing interest owing to their production cost and high energy conversion efficiency. They are a potential alternative to silicon-based photovoltaic devices [1] . The total photoelectric conversion efficiency of DSSCs has already been enhanced to 13.1% till now [2] .
For a DSSC to be functional, dye molecules have to be attached to the TiO 2 particle surface. The molecules absorb light, and this excites electrons to higher levels from their ground states. The electrons then pass into the conduction band of TiO 2 . Thereafter, they percolate through the nanoporous TiO 2 structure to a transparent conducting film, flowing through an external load to the counter electrode [2 , 3] .
The extent of conversion efficiency increase has been limited owing to recombination between electrons and either oxidized dye molecules or electron-accepting species in the electrolyte during the charge transport process (2e + I 3 → 3I ) [4 - 7] . Recently, this charge recombination has been significantly suppressed by employing thin blocking layers such as those of TiO 2 , Nb 2 O 5 , and ZnO for semiconductors, and CaCO 3 and BaCO 3 for insulating materials [8 - 12] .
As is already known, SiO 2 is a useful material in the microelectronics industry and for thin electroluminescence devices. In researches on electroluminescence devices, it was found that an inserted SiO 2 film can remarkably enhance their light extraction efficiency. Sheng et al. [13] exhibited 11.8% enhancement in light output power by inserting a SiO 2 current blocking layer (CBL). In addition, Deng et al. [14] increased the efficiency by a factor of two by inserting a SiO 2 layer between ITO and the hole-transport layer. However, not many systematic studies have been undertaken to investigate the modification of photoelectric properties by the addition of SiO 2 blocking layers.
The overall objective of this research was to evaluate the optical, structural, and photoelectrochemical properties of ITO with different thicknesses of SiO 2 used as a buffer and blocking layer in order to obtain high energy conversion efficiency from DSSCs.
2. EXPERIMENTS
- 2.1 Preparation of electrodes
Prior to the experiments, EMP (essential macleod program) was selected to estimate the experimental results. The refractive indexes of all materials were measured using an ellipsometer (UNISEL/M200 with 64CH MWL, HORIBA) to perform an accurate optical simulation. ITO/SiO 2 multilayer films were deposited on a soda-lime substrate by DC/RF magnetron sputtering. For the sputtering, high-purity SiO 2 ceramic targets (99.99%) and ITO targets (99.99%, In 2 O 3 :SnO 2 = 90:10 wt%) were used. Sputtering was performed at a substrate temperature of 500℃ in an argon atmosphere with a target-to-substrate distance of 55 mm. The experimental deposition conditions are listed in Table 1 . The ITO thickness layer was kept constant at 370 nm. As a blocking layer, SiO 2 layers with thicknesses of 0.1, 0.5, 1, and 5 nm were deposited. Additionally, FTO glass with 8 Ω/sq. (Dyesol-Timo) was prepared for property comparison with the ITO electrode used. Transmittance of the multilayer films was measured using a spectrophotometer (Konica Minolta). Further, the sheet resistances of the films were measured using a four-point probe.
Fabrication of optical thin films by using RF/DC magnetron sputtering method.
PPT Slide
Lager Image
Fabrication of optical thin films by using RF/DC magnetron sputtering method.
- 2.2 Fabrication of DSSCs
Mesoscopic TiO 2 films were prepared via the screen printing method by using TiO 2 paste (Solaronix, BN 376c/211013 FM), which is suitable for low-temperature sintering. After screenprinting, the prepared films were sintered under airflow at 150℃ for 30 min. The final thickness of the TiO 2 films was approximately 8.9 μm. To adsorb a photosensitized dye on the TiO 2 surface, the films were immersed in a Ru complex dye (N719) for 24 h at room temperature. Then, Pt-treated ITO films, which were used as counter electrodes, were placed over the dye-coated films and edges of the cells were sealed with 0.5-mm-wide strips of 60-μm-thick Surlyn (Solarnix, SX 1170, Hot Met). After sealing, an iodide-based electrolyte, tri-iodide in acetonitrile (Solaronix, AN-50), was injected into the cell through two small holes drilled in the counter electrode. The holes were then covered with a small cover glass and sealed. For DSSCs with FTO glass, the experimental methods were the same as those used in the case of DSSCs with the ITO electrode. Fig. 1 shows a schematic view of the interfaces in the DSSCs.
PPT Slide
Lager Image
Schematic view of interfaces in DSSCs.
The crystal structure of the films was analyzed by X-ray diffractometry (XRD; Rigaku). The film morphology was observed by field-emission scanning electron microscopy (FE-SEM; JEOL). Atomic force microscopy (AFM) were conducted to study the surface roughness using the model Nanoscope IIIa (Digital Instruments). The photocurrent-voltage (I-V) characteristics of the DSSCs were measured under conditions of AM 1.5 and 100 mW/m 2 (1 sun) by using a solar simulator.
3. RESULTS AND DISCUSSION
- 3.1 Structural properties
Figure 2 shows the XRD patterns for the ITO, FTO, and TiO 2 nanoporous films annealed at 150℃ for 30 min.
PPT Slide
Lager Image
XRD patterns for (a) TiO2 nanoporous film, (b) FTO film, and (c) ITO film annealed at 150℃ substrate temperature.
The diffraction pattern shown in Fig. 2(a) clearly indicates a tendency for crystallinity in the TiO 2 nanoporous film with a (101) preferred orientation at 2 θ = 26.24°.
Usually, the anatase phase of TiO 2 thin films is formed at temperatures above 250℃ and is then transformed into the rutile phase between 700 and 900℃ [15] . In our XRD experiments, the TiO 2 nanoporous films calcined at 150℃ exhibited an anatase phase, even those sintered at a low temperature of 150℃. Thus, the films were crystalline. As shown in Fig. 2(b) , the FTO film showed a tendency for crystallinity with a (110) preferred orientation at 2 θ = 12.44°. Further, as can be seen in Fig. 2(c) , the ITO film too showed a tendency for crystallinity with (222) and (400) preferred orientations at 2 θ = 30.18° and 35.18°, respectively. Fig. 3 shows the cross-sectional SEM images of ITO, FTO, and TiO 2 nanoporous films. From Fig. 3(a) , the thickness of the TiO2 nanoporous film was calculated to be approximately 8.9 μm.
PPT Slide
Lager Image
Cross-sectional SEM images of (a) TiO2 nanoporous film, (b) ITO film, and (c) FTO film.
The thickness of ITO and FTO films ( Figs. 3(b) and (c) ) was 377 nm and 860 nm, respectively. In case of the ITO film, the measured film thickness well matched the simulated result (λ 1.5 = 370 nm) obtained by EMP.
Figure 4 demonstrates the FE-SEM images of (a) bare ITO and ITO films with different thicknesses of the SiO 2 thin film: (b) 0.1 nm, (c) 0.5 nm, (d) 1 nm, and (e) 5 nm. The scale bar indicates 1 μm, and grain size was varied from 5 nm to 10 nm. By increasing the SiO 2 film thickness from 0.1 nm to 0.5 nm ( Figs. 4(b) and (c) ), the grain size gradually increased to around 3 nm. However, the grain size continuously decreased thereafter upon further increasing the SiO 2 film thickness from 0.5 nm to 5 nm ( Figs. 4(c) - (e) ).
PPT Slide
Lager Image
Surface FE-SEM images of (a) bare ITO substrate, and ITO substrate with different SiO2 thin film thicknesses: (b) 0.1 nm, (c) 0.5 nm, (d) 1 nm, and (e) 5 nm.
Since the SiO 2 layer was too thin, its thickness could not be confirmed by cross-sectional FE-SEM images and was therefore calculated on the basis of the deposition rate of the SiO 2 thin film.
- 3.2 Optical properties
Table 2 lists the summarized results for the refractive index n and extinction coefficient k for ITO and SiO 2 thin films in the visible range, calculated using ellipsometry. The refractive indexes of ITO and SiO 2 thin films were 2.03 and 1.625; these values are higher than the theoretical values. Further, the measured extinction coefficients of ITO and SiO 2 were 0.011 and 0.014, respectively.
Comparison of physical properties of ITO and SiO2in visible range.
PPT Slide
Lager Image
Comparison of physical properties of ITO and SiO2 in visible range.
Fig. 5 shows a comparison of the spectral transmittance of various multilayer thin films on the basis of simulated and experimental data.
PPT Slide
Lager Image
Comparison of spectral transmittance of ITO/SiO2 multilayer thin films on the basis of (a) simulated and (b) experimental data.
Figure 5(a) shows the simulation results for the optical transmittance of the ITO/SiO 2 multilayer films, calculated using EMP, as a function of the SiO 2 thickness. As can be seen in Fig. 5(a) , the multilayer films had high transparency in the visible range of 400~700 nm and the transmittance of the ITO/SiO 2 thin film slightly increased with increasing thickness of the SiO 2 thin film. Fig. 5(b) shows the measured optical transmittance of the ITO/SiO2 multilayer films as a function of the SiO2 thickness. The transmittance of the ITO film was 81% at 550 nm wavelength. Some distinct differences were observed between the experimental and simulated results. The experimentally measured transparency appeared to be somewhat higher than that obtained via simulation for wavelength values below 525 nm. On the other hand, the transparency of obtained from experimental results was lower than that obtained through simulation for wavelength values above 525 nm. This might be attributed to light scattering on the ITO film surface and interface instability due to diffusion. Moreover, the substrate temperature was also considered to cause differences between the experimental and EMP simulation results.
As seen in Fig. 5(b) , the transmittance of the FTO film was lower (approximately 10%) than that of all the ITO films. In particular, the transmittance of the ITO film was much higher (up to 23%) than that of the FTO film at wavelengths below 500 nm, where photoelectrodes loaded with the N719 dye absorbed light sufficiently [17] to consume the incident light within the increased light path. Since the ITO film could enhance incident light, short-circuit current ( J sc ), which is related to photovoltaic efficiency, was enhanced by photovoltaic generation in the nanoporous TiO 2 film.
- 3.3 Photovoltaic performance of DSSCs
Figure 6 shows the photocurrent density-voltage ( J - V ) curves for DSSCs obtained under 100 mW/m 2 illumination with AM 1.5.
PPT Slide
Lager Image
Photocurrent-voltage curves for DSSCs made of FTO film, ITO film, and ITO films with various SiO2 thin film thicknesses.
The characteristic parameters for DSSCs can be obtained from the photocurrent density-voltage curve; these parameters are short-circuit current ( J sc ), open-circuit voltage ( V oc ), fill factor ( FF ), and conversion efficiency ( η ).
The efficiency ( η ) of DSSCs can be calculated from the following equation:
PPT Slide
Lager Image
where J sc is the integral photocurrent density (current obtained under short-circuit conditions divided by the area of the cell), V oc is the open-circuit voltage, FF is the fill factor ( FF = (I × V)max / I sc V oc ; related to the series resistance for potential solar cells), and P in is the intensity of incident light. The characteristic parameters for DSSCs corresponding to Fig. 6 are summarized in Table 3 .
Comparison of characteristic parameters for DSSCs with thin films.
PPT Slide
Lager Image
Comparison of characteristic parameters for DSSCs with thin films.
The DSSC fabricated on the bare ITO film showed a V oc of 0.697 V, J sc of 10.596 mA/cm 2 , FF of 66.423, and calculated power conversion efficiency ( η AM1.5 ) of 4.909%. Compared with the DSSC fabricated on the bare FTO film, η and J sc of the DSSC with the bare ITO film were higher by 29.1% and 45%, respectively. However, V oc of the latter was slightly diminished by 5.4%. The enhancement of J sc can be attributed to the increase in photovoltaic generation in the nanoporous TiO 2 film.
The DSSC with the 0.1-nm-thick SiO 2 deposited ITO film showed the maximum efficiency with 5.259%, V oc of 0.68 V, J sc of 11.48 mA/cm 2 , and FF of 66.65. We assume that the enhancement of J sc in the DSSC with the blocking layer was due to the increase in protection provided by the blocking layer against the ionic penetration of the electrolyte. The DSSC with the 0.5-nm-thick SiO 2 deposited ITO film exhibited similar parameter values as the DSSC with the bare ITO film. However, the efficiency of the DSSCs deposited over the 1-nm-thick SiO 2 film sharply decreased.
Consequently, the cell performance of DSSCs under illumination seems to indicate a decrease in the recombination rate in the cells, when the 0.1-nm-thick SiO 2 film was used as the blocking layer.
Figure 7 shows the Nyquist plots of DSSCs with the bare ITO film, and ITO films with various thicknesses of the SiO 2 thin film. As can be seen in the figure, two semicircles were obtained in the Nyquist plots. The larger semicircle in the frequency range 10 3 -10 Hz corresponds to the recombination resistance ( R 2 ) and chemical capacitance ( C 2 ) across the TiO 2 /redox electrolyte interface. The smaller semicircle in the frequency range 1 KHz-1 MHz corresponds to charge-transfer resistance ( R 1 ), and the capacitance ( C 1 ) should be ascribed to the process occurring at the interface of the redox electrolyte/Pt counter electrode [18]. The DSSC based on the ITO film with the 0.1-nm-thick SiO 2 layer showed the lowest value of R 1 ; this might be due to the blocking of charge recombination.
PPT Slide
Lager Image
Nyquist plot of DSSCs with bare ITO film, and those with ITO films containing SiO2 thin films of various thicknesses.
Analysis of the data obtained revealed that the ITO film resistance increased with increasing SiO 2 thickness, and this provided supporting evidence for the FF decrease. This result is in good agreement with the J-V data.
4. CONCLUSIONS
In summary, the characteristics of the RF/DC sputtering grown bare ITO film and ITO films with SiO 2 blocking layers of various thicknesses were systematically investigated. Compared with the DSSC fabricated on the bare FTO film, the conversion efficiency ( η ) and short-circuit current ( J sc ) of the DSSC with the bare ITO film were higher by 29.1% and 45%, respectively.
The DSSC based on the ITO film with the 0.1-nm-thick SiO 2 blocking layer showed the maximum efficiency with 5.4%. This result is in good agreement with the Nyquist data. Finally, the use of the 0.1-nm-thick SiO 2 blocking layer increased the overall efficiency of the DSSC by up to 7.1%.
References
Mendizabal F. , Lopéz A. , Arratia-Pérez R. , Zapata-Torres G. (2015) Computational & Theoretical Chemistry [DOI: ] 1070 117 -
Shen P. S. , Tseng C. M. , Kuo T. C. , Shih C. K. , M. H. Li , Chen P. (2015) Solar Energy [DOI: ] 120 345 -
Wang Z. , Tang Q. , He B. , Chen H. , Yu L. (2015) Electrochimica Acta [DOI: ] 178 18 -
Cisneros R. , Beley M. , Fauvarque J. F. , Lapicque F. (2015) Electrochimica Acta [DOI: ] 171 49 -
Kumar R. , More V. , Mohanty S. P. , Nemala S. S. , Mallick S. , Bhargava P. (2015) Journal of Colloid and Interface Science [DOI: ] 459 146 -
Wang X. , Zhang Y. , Xu Q. , Xu J. , Wu B. , Gong M. , Chu J. , Xiong S. (2015) J. Photoch. Photobio. A: Chemistry 311 112 -
Mehmood U. , Hussein I. A. , Harrabi K. , Mekki M. B. , Ahmed S. , Tabet N. (2015) Sol. Energ. Mat. Sol. C. [DOI: ] 140 174 -
Duong T. T. , Choi H. J. , Yoon S. G. (2014) J. Alloys Comp. [DOI: ] 591 1 -
Chen J. , Wang J. , Bai F. Q. , Hao L. , Pan Q. J. , Zhang H. X. (2013) Dyes and Pigments [DOI: ] 99 201 -
Cho T. Y. , Ko K. W. , Yoon S. G. , Sekhon S. S. , Kang M. G. , Hong Y. S. , Han C. H. (2013) Curr. Appl. Phys. [DOI: ] 13 1391 -
Zhou S. , Liu S. , Ding H. (2013) Surface Optics & Laser Technology [DOI: ] 47 127 -
Li B. H. , Tang Y. W. , Luo L. J. , Xiao T. , Li D. W. , Hu X. Y. , Yuan M. (2010) Appl. Surf. Sci. [DOI: ] 257 197 -
Aidla A. , Iistare T. , Kiisler A. A. , Aarik J. , Sammelselg V. (1997) Thin Solid Films [DOI: ] 305 270 -
Kumagai H. , Toyoda K. , Matsumoto M. , Obara M. , Suzki M. (1994) Thin Solid Films 263 2945 -
Fisher A. C. , Peter L. M. , Ponomarev E. A. , Walker A. B. , Wijayantha K.G.U. (2000) J. Phys. Chem. B [DOI: ] 104 949 -