Conical islands of TiO2 nanotube arrays in the photoelectrode of dye-sensitized solar cells
© Kim et al.; licensee Springer. 2015
Received: 25 November 2014
Accepted: 6 January 2015
Published: 11 February 2015
Ti conical island structures were fabricated using photolithography and the reactive ion etching method. The resulting conical island structures were anodized in ethylene glycol solution containing 0.25 wt% NH4F and 2 vol% H2O, and conical islands composed of TiO2 nanotubes were successfully formed on the Ti foils. The conical islands composed of TiO2 nanotubes were employed in photoelectrodes for dye-sensitized solar cells (DSCs). DSC photoelectrodes based on planar Ti structures covered with TiO2 nanotubes were also fabricated as a reference. The short-circuit current (J sc) and efficiency of DSCs based on the conical island structures were higher than those of the reference samples. The efficiency of DSCs based on the conical island structures reached up to 1.866%. From electrochemical impedance spectroscopy and open-circuit voltage (V oc) decay measurements, DSCs based on the conical island structures exhibited a lower charge transfer resistance at the counter cathode and a longer electron lifetime at the interface of the photoelectrode and electrolyte compared to the reference samples. The conical island structure was very effective at improving performances of DSCs based on TiO2 nanotubes.
Dye-sensitized solar cells (DSCs) have received great interest as promising alternatives to conventional silicon solar cells . Their low cost and easy fabrication processes are powerful advantages. For example, DSCs can be fabricated without the high-cost vacuum equipment required for Si cells, such as plasma-enhanced chemical vapor deposition (PECVD) and atomic layer deposition (ALD). Wet etching processes, such as saw damage etching and texturing, which are widely used in the fabrication of Si solar cells, are not required in DSCs, which simplifies their fabrication.
Gratzel and O’Regan achieved remarkably high-efficiency DSCs by using mesoporous TiO2 nanoparticle-based films . Recently, Burschka et al. reported high efficiency, up to 15%, by fabricating inorganic-organic hybrid solar cells containing perovskite compounds . However, the efficiencies of DSCs are still too low for commercialization compared with conventional Si solar cells.
The main components which affect the performance of DSCs are the dyes [3-13], photoelectrodes [14-38], counter cathodes [39-46], and electrolytes [47-51]. Among these components, increasing the surface area of the photoelectrodes and reducing charge recombination between the photoelectrodes and electrolytes are critical factors in improving the efficiencies of DSCs.
TiO2 nanoparticle structures have been widely used for the photoelectrodes of DSCs. However, structural defects which exist at the contacts between the TiO2 nanoparticles not only hinder electronic diffusion across TiO2 nanocrystalline films but also act as charge recombination sites [20-22,24,26]. To address this issue, TiO2 nanostructures such as nanowires [31,33,34], nanotubes [20-30,37,38,52,53], nanohemispheres [35,36], and nanoforests  have been applied to the photoelectrodes of DSCs as alternatives to the conventional TiO2 nanoparticle structure.
Of these nanostructures, the TiO2 nanotube has received a great deal of attention due to its one-dimensional charge transport. Charge percolation in TiO2 nanotube-based films is easier than that in TiO2 nanoparticle-based films [20-22]. It has been reported that electron lifetimes in TiO2 nanotube-based films are longer than those in TiO2 nanoparticle-based films .
In this study, conical island shapes were patterned on a Ti substrate to increase the specific surface area for dye adsorption. Ti surfaces with these conical islands were anodized, and TiO2 nanotube arrays were formed on the entire Ti surface. Conical islands composed of TiO2 nanotubes were successfully fabricated and applied as the photoelectrodes of DSCs. Planar Ti photoelectrodes were also prepared with TiO2 nanotube arrays, and then the characteristics and performance of the conical island photoelectrode structure were compared with those of the planar photoelectrode structure. To our knowledge, this is the first trial to report the fabrication of conical islands composed of TiO2 nanotubes and their application to DSCs.
The experimental procedures for making conical islands composed of TiO2 nanotubes are very similar to those found in our previous report . To make conical islands on the surface of 0.5-mm-thick Ti foils (99%, Alfa Aesar Co., Ward Hill, MA, USA), 5-μm-thick photoresists (PR; L-300, Dongjin Co., Hwaseong-si, South Korea) were coated on the surface of Ti foils using a spin-coater (Mark-8 Track, TEL Co., Tokyo, Japan). The spin-coated photoresists were softly baked at 120°C for 120 s and hardly baked at 110°C for 5 min. A dot-patterned photomask was used to make PR patterning by UV light exposure. The UV light, which had an energy of 14.5 mJ/s, was illuminated for 5 s, and the PR was developed. The PR in the UV-unexposed area was removed.
The PR-patterned Ti foil was dry-etched at 25°C for 40 min by using reactive ion etching (RIE) equipment (ICP380, Oxford Co., Abingdon, Oxfordshire, UK). BCl3 and Cl2 gases were used in the RIE process with a top power of 800 W and a bottom power of 150 W. Photoresists on the UV-exposed area played a role in protecting the flat Ti surface during the RIE process. Only the Ti surface in the UV-unexposed area was etched out. The remaining photoresists after the RIE process were stripped at 250°C for 20 min using a photoresist stripper (TS-200, PSK Co., Hwaseong-si, South Korea). O2 and N2 gases were used for photoresist stripping with a power of 2,500 W.
To obtain a proper microstructure of TiO2 nanotube arrays, anodic oxidation voltages and times applied by a DC power supply were computer-controlled by a LabVIEW program. The ethylene glycol solution included 0.5 wt% NH4F and 0.2 vol% H2O. A constant potential of 60 V with a ramping speed of 1 V/s was applied between the anode and the cathode. Pt metal was used as a counter cathode. Anodizing time was varied to control the optimum thickness of TiO2 nanotubes in the conical islands. As-anodized TiO2 nanotubes were rinsed with DI water and annealed at 500°C for 1 h. The morphologies of the conical islands composed of TiO2 nanotubes were studied by field emission scanning electron microscopy (FESEM; Hitachi SU-70, Hitachi, Ltd., Chiyoda-ku, Japan) at Korea Basic Science Institute. As-anodized and annealed TiO2 nanotubes were analyzed by X-ray diffraction (XRD; Rigaku D/MAX-RC, Shibuya-ku, Japan, Cu Kα radiation) to confirm their crystallization.
The Ti substrates with conical islands composed of TiO2 nanotubes were then prepared for use as the photoelectrodes of DSCs. The TiO2 photoelectrodes were immersed at room temperature for approximately 1 day in an ethanol solution containing 3 × 10−4 M cis-bis(isothiocyanato)bis(2,2′bipyridyl-4,4′dicarboxylato) ruthenium(II) bis-tetrabutylammonium (N719) dye. The dye-adsorbed photoelectrodes were rinsed with ethanol solution and were dried at room temperature. Pt-coated fluorine-doped tin oxide (FTO) glasses were prepared as counter electrodes by spin coating 0.7 mM H2PtCl6 solution in 2-propanol at 500 rpm for 10 s and subsequently annealing at 380°C for 30 min. The dye-adsorbed photoelectrodes and Pt-coated FTO glasses were spaced by using 60-μm Surlyn film purchased from DuPont Co., Ltd. (Wilmington, DE, USA). The liquid electrolyte was prepared by dissolving 0.6 M 1-hexyl-2,3-dimethylimidazolium iodide (C6DMIm), 0.05 M iodine, 0.1 M lithium iodide, and 0.5 M 4-tert-butylpyridine in 3-methoxyacetonitrile. Current-voltage (J-V) characteristics were measured under AM 1.5G condition (Keithley Model 2400 source measure unit, Keithley Instruments, Inc., Cleveland, OH, USA). Electrochemical impedance spectroscopy (EIS) behaviors were analyzed at open-circuit condition and in the frequency range of 100 kHz to 100 mHz. A 1,000-W xenon lamp (Oriel, 91193, Newport Co., Stratford, CT, USA) was used as a light source for one sun condition.
Results and discussion
However, photoresists have weaker cross-linking at an edge than at the center. At edges, cross-linked photoresists can be easily damaged during the RIE process if the etching time is long enough. In that case, the cross-linked photoresists at the edge areas can be crushed by the reactive ions after the formation of the Ti protruded cylinders. This allows the protruded cylinders to be converted into conical islands by increasing the dry etching time, as shown in Figure 2a.
The top and the bottom of the produced conical islands have diameters of approximately 1 μm and approximately 4 μm, respectively. The height of the conical islands is approximately 5 μm. Ti conical island arrays can be seen in Figure 2b. The distance between adjacent conical islands is approximately 8 μm and coincides with the photomask patterns.
For experimental purposes, both types of TiO2 arrays were prepared with nanotube lengths of 1.0, 1.5, and 2.0 μm. Both types of photoelectrodes were fabricated with the identical active cell size of 5 mm × 5 mm. The photoelectrode with the planar TiO2 nanotube arrays was later used as a reference sample to compare J-V characteristics and EIS behaviors with the conical island structure.
J - V characteristics of DSCs based on planar and conical island structures of TiO 2 nanotube arrays
J sc (mA/cm 2 )
V oc (V)
Planar structure, 1.0 μm
1.159 ± 0.104
Planar structure, 1.5 μm
1.147 ± 0.167
Planar structure, 2.0 μm
1.378 ± 0.092
Conical island structure, 1.0 μm
1.598 ± 0.067
Conical island structure, 1.5 μm
1.774 ± 0.21
Conical island structure, 2.0 μm
1.866 ± 0.279
For the same length of TiO2 nanotubes, DSCs based on the conical island structure show higher J sc than DSCs based on the planar structure. The added TiO2 nanotube arrays on the inclined surfaces of the conical island further increase the surface area available to adsorb the dyes and produce photoelectrons.
DSCs having 2.0-μm-long TiO2 nanotube arrays showed the best performances for both planar and conical island structures. The short-circuit current and efficiency for the conical island structures and 2.0-μm-long TiO2 nanotubes were 5.877 mA/cm2 and 1.866%, respectively. In all cases, the efficiencies of the conical island structure DSCs were higher than those based on the planar structure. The conical island structure was very effective at improving DSC power conversion efficiency. It is also anticipated that conical island structures with TiO2 nanotube arrays longer than 2.0 μm will have still higher efficiency.
Chemical resistances in Figure 7a include the charge transfer resistance (R Pt/electrolyte) at the interface between the Pt counter electrode and electrolyte, charge transfer resistance (R TiO2/electrolyte) at the interface between the TiO2 photoelectrode and electrolyte, and charge transport resistance (R electrolyte) in the electrolyte. DSCs based on the conical island structure have lower chemical resistance due to remarkably decreased R Pt/electrolyte. The reason for this decrease in R Pt/electrolyte is not clear. It seems that the conical island may be a better structure for transferring electrons to the counter electrode than the planar structure, since the J sc of the conical island structure is higher than that of the planar structure.
Figure 7b shows Bode plots of DSCs based on planar and conical island structures. Usually, Bode plots of DSCs have three main phase (θ) peaks, according to the frequency range. The high-frequency (1 kHz to 100 kHz) region is attributed to charge transfer at the interface between the counter cathode and electrolyte. The medium-frequency (1 Hz to 1 kHz) region is the response of charge transfer at the interface between the TiO2 photoelectrode and electrolyte. The low-frequency (1 mHz to 1 Hz) region reflects charge transport associated with the Nernstian diffusion process in the electrolyte. If the frequency at the phase peaks can be determined, the electronic lifetimes at each interface and in the electrolyte can be calculated by just inversing the peak frequencies. Only two phase peaks, in the high- and medium-frequency regions, could be found in Figure 7b. The phase peak in the low-frequency region was not observed because the acquisition time was too short to obtain the diffusion peak.
In the high-frequency region, frequencies at the phase peaks are approximately 2.1 kHz and approximately 2.4 kHz for DSCs based on planar and conical island structures, respectively; therefore, the electronic lifetimes are 0.476 and 0.417 ms, respectively. On the other hand, in the medium-frequency region, the frequencies at phase peaks are 10 and 5.5 Hz for DSCs with planar and conical island structures; thus, the electronic lifetimes are 0.1 and 0.18 s, respectively. The difference of electronic lifetimes in the high-frequency region is negligible; however, in the medium-frequency region, the electronic lifetime of DSCs based on the conical island structure is obviously longer than that of DSCs based on the planar structure. These results indicate that conical islands composed of TiO2 nanotubes are more effective for charge transfer at the interface between the TiO2 photoelectrode and electrolyte.
Ti conical islands were fabricated by coating photoresists on Ti foils, stacking dot-patterned photomasks on the photoresists, illuminating with UV light, etching the surface with the RIE method, and stripping the photoresist. When the produced Ti conical islands were anodized, conical islands composed of TiO2 nanotubes were successfully fabricated. The conical islands composed of TiO2 nanotubes were then employed as photoelectrodes of DSCs. The J-V characteristics of DSCs based on the conical island structures were compared with those of DSCs based on the planar structures covered with TiO2 nanotubes. The J sc and the efficiency of DSCs based on the conical island structures were higher than those of DSCs based on the planar structures. The efficiency of the DSCs using conical island structures reached 1.87%. The charge transfer resistance at the counter cathode of DSCs based on the conical island structures was remarkably reduced compared to that of DSCs based on the planar structures. The electron lifetime at the interface between the photoelectrode and electrolyte was longer for DSCs based on the conical island structure than that for DSCs based on the planar structure. The conical island structure effectively enhanced the performance of DSCs based on TiO2 nanotube arrays. The relatively low efficiency of DSCs based on the conical island structure compared with that of typical DSCs can be overcome by controlling the microstructure of the conical island, dye, electrolyte, surface treatment of TiCl4, and so on.
This research was financially supported by the Ministry of Education, Science and Technology (MEST) and by the National Research Foundation of Korea (NRF) through the Human Resource Training Project for Regional Innovation (Grant No. 2012H1B8A2026009).
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