# Dye-Sensitized Solar Cells Based onBi4Ti3O12

Authors: Zeng Chen; Shengjun Li; Weifeng Zhang
Journal: International Journal of Photoenergy
 (2011)

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## Abstract

Bismuth titanate (Bi4Ti3O12) particles were synthesized by hydrothermal treatment and nanoporous thin films were prepared on conducting glass substrates. The structures and morphologies of the samples were examined with X-ray diffraction and scanning electron microscope (SEM). Significant absorbance spectra emerged in visible region which indicated the efficient sensitization of Bi4Ti3O12 with N3 dye. Surface photovoltaic properties of the samples were investigated by surface photovoltage. The results further indicate that N3 can extend the photovoltaic response range of Bi4Ti3O12 nanoparticles to the visible region, which shows potential application in dye-sensitized solar cell. As a working electrode in dye-sensitized solar cells (DSSCs), the overall efficiency reached 0.48% after TiO2 modification.


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## Body

## 1.  Introduction

Dye-sensitized solar cells (DSSCs) have attracted the attention of scientists all over the world because of their relatively high efficiency and low-cost production [1, 2]. In dye-sensitized solar cells, the most important part is the nanoporous electrode made of wideband gap semiconductor for supporting dye molecules and transporting photo-injected electrons. Previous research has been limited to simple binary oxides, including TiO2, ZnO [3], SnO2 [4], Nb2O5 [5], WO3 [6], and In2O3 [7], and so forth. Little attention has been carried out on the ternary oxides, except for SrTiO3 [8] and Zn2SnO4 [9]. However, the multication oxides show more advantages for the tuning of materials’ chemical and physical properties by altering the compositions [10, 11]. It is interesting to investigate the potential applications of new ternary oxides in DSSCs for higher photoelectric conversion efficiency.Bismuth titanate, Bi4Ti3O12, behaves as an n-type semiconductor with an indirect band gap of 3.2 eV [12, 13]. It is an important ceramic material widely studied on its nonvolatile memory, optical memory, piezoelectric, and photocatalytic properties [14–17]. Its photovoltaic properties, however, have scarcely been reported. In the previous work, we have investigated the surface photovoltage response of thin compact Bi4Ti3O12 film on fluorine-doped tin oxide conductive glass substrate [13]. In this work, nanoporous Bi4Ti3O12 electrode was prepared and sensitized with N3 dye and the photoelectric properties was investigated.


## 2. Experimental

### 2.1. Preparation and Characterization of Nanocrystal Bi4Ti3O12 Electrode

Bi(NO3)3·5H2O and Ti(OC4H9)4 were used as the bismuth and titanium sources, respectively, for the hydrothermal synthesis of Bi4Ti3O12. The two sources were dissolved in glacial acetic acid to form two transparent solutions. A little acetylacetone were added as stabilizer. Then, bismuth nitrate solution was slowly added to the tetrabutyl titanate solution. Eight percent excess Bi(NO3)3·5H2O was added to compensate for the Bi loss during the thermal annealing. After magnetic stirring for 24 hours, sodium carbonate (Na2CO3) aqueous solution was added dropwise to the mixture under vigorous stirring to form a yellow colloid. The mixture was autoclaved at 190°C for 12 h. The resulting precipitates were ultrasonic dispersed and washed thoroughly with deionized water and ethanol successively, then dried at 60°C in an oven. The sample was sintered at 690°C for two hours to form Bi4Ti3O12.Bi4Ti3O12 particles were suspended, mixing 0.6 g with 0.1 g of ethylcellulose in 5 mL of 1-butanol. Thin porous Bi4Ti3O12 films were prepared by spreading the suspension onto conducting glass substrates (30 Ω/□), followed by heating at 450°C for 30 min in air to eliminate the ethylcellulose. TiO2 coated Bi4Ti3O12 was also prepared by adding tetrabutyl titanate to the colloid of Bi4Ti3O12 in 1-butanol before the doctor blading process.The crystalline phases of the samples were characterized by DX-2500 X-ray diffractometer (XRD) with a monochromatized Cu Kα irradiation (λ=0.154145 nm). The morphologies of the samples were determined using a HitachiS-4300F field emission scanning electron microscope (SEM). The absorption spectrum was measured by a UV-vis-NIR photospectrometer (Varian Cary 5000). To investigate the charge separation behavior at the surface of the samples, the surface photovoltage spectroscopy (SPS) was carried out with a home-built apparatus including a 500 W xenon lamp (CHF XQ500 W), a double-grating monochromator (Zolix SP500), a lock-in amplifier (SR830-DSP), a light chopper (SR540), and so on [18].


### 2.2. Fabrication and Characterization of Dye-Sensitized Solar Cells

Nanoporous Bi4Ti3O12 films were dipped into the 5 × 104 mol ethanol solution of cis-bis(thiocyanato)-N,N′-bis(2,2′-bipyridyl-4,4′-dicarboxylate) ruthenium (II) (N3 dye) for more than 48 h to absorb enough sensitizer. The counter electrode was Pt foil. The mixture of 0.6 M dimethylpropylimidazolium iodide, 0.1 M iodine, 0.5 M 4-tertbutylpyridine, and 0.1 M lithium iodide in methoxy acetonitrile was selected to be the electrolyte of DSSCs. The counter electrode and the dye-sensitized Bi4Ti3O12 electrode were clamped firmly together. The redox electrolyte solution was introduced into the porous nanocrystalline Bi4Ti3O12 film by capillary action.The photoelectrochemical characteristics of DSSCs were measured by the photocurrent-voltage curve (I-Vcurves) measurement with an Electrochemical Workstation (Shanghai Chen-hua Instrument Co, China) under the simulated solar light. A 500 W xenon lamp was used as the light source. The incident light intensity was 100 mW·cm−2 measured by a Radiation Meter (FZ-A, Beijing Normal University, China) and the active cell area was 0.25 cm2. The flat band potential was measured by the Mott-Schottky analysis method with the potential range from 0 to 1.0 V [19, 20].


## 2.1. Preparation and Characterization of Nanocrystal Bi4Ti3O12 Electrode

Bi(NO3)3·5H2O and Ti(OC4H9)4 were used as the bismuth and titanium sources, respectively, for the hydrothermal synthesis of Bi4Ti3O12. The two sources were dissolved in glacial acetic acid to form two transparent solutions. A little acetylacetone were added as stabilizer. Then, bismuth nitrate solution was slowly added to the tetrabutyl titanate solution. Eight percent excess Bi(NO3)3·5H2O was added to compensate for the Bi loss during the thermal annealing. After magnetic stirring for 24 hours, sodium carbonate (Na2CO3) aqueous solution was added dropwise to the mixture under vigorous stirring to form a yellow colloid. The mixture was autoclaved at 190°C for 12 h. The resulting precipitates were ultrasonic dispersed and washed thoroughly with deionized water and ethanol successively, then dried at 60°C in an oven. The sample was sintered at 690°C for two hours to form Bi4Ti3O12.Bi4Ti3O12 particles were suspended, mixing 0.6 g with 0.1 g of ethylcellulose in 5 mL of 1-butanol. Thin porous Bi4Ti3O12 films were prepared by spreading the suspension onto conducting glass substrates (30 Ω/□), followed by heating at 450°C for 30 min in air to eliminate the ethylcellulose. TiO2 coated Bi4Ti3O12 was also prepared by adding tetrabutyl titanate to the colloid of Bi4Ti3O12 in 1-butanol before the doctor blading process.The crystalline phases of the samples were characterized by DX-2500 X-ray diffractometer (XRD) with a monochromatized Cu Kα irradiation (λ=0.154145 nm). The morphologies of the samples were determined using a HitachiS-4300F field emission scanning electron microscope (SEM). The absorption spectrum was measured by a UV-vis-NIR photospectrometer (Varian Cary 5000). To investigate the charge separation behavior at the surface of the samples, the surface photovoltage spectroscopy (SPS) was carried out with a home-built apparatus including a 500 W xenon lamp (CHF XQ500 W), a double-grating monochromator (Zolix SP500), a lock-in amplifier (SR830-DSP), a light chopper (SR540), and so on [18].


## 2.2. Fabrication and Characterization of Dye-Sensitized Solar Cells

Nanoporous Bi4Ti3O12 films were dipped into the 5 × 104 mol ethanol solution of cis-bis(thiocyanato)-N,N′-bis(2,2′-bipyridyl-4,4′-dicarboxylate) ruthenium (II) (N3 dye) for more than 48 h to absorb enough sensitizer. The counter electrode was Pt foil. The mixture of 0.6 M dimethylpropylimidazolium iodide, 0.1 M iodine, 0.5 M 4-tertbutylpyridine, and 0.1 M lithium iodide in methoxy acetonitrile was selected to be the electrolyte of DSSCs. The counter electrode and the dye-sensitized Bi4Ti3O12 electrode were clamped firmly together. The redox electrolyte solution was introduced into the porous nanocrystalline Bi4Ti3O12 film by capillary action.The photoelectrochemical characteristics of DSSCs were measured by the photocurrent-voltage curve (I-Vcurves) measurement with an Electrochemical Workstation (Shanghai Chen-hua Instrument Co, China) under the simulated solar light. A 500 W xenon lamp was used as the light source. The incident light intensity was 100 mW·cm−2 measured by a Radiation Meter (FZ-A, Beijing Normal University, China) and the active cell area was 0.25 cm2. The flat band potential was measured by the Mott-Schottky analysis method with the potential range from 0 to 1.0 V [19, 20].


## 3. Results and Discussion

### 3.1. Structures and Morphologies

The XRD pattern of the as-prepared Bi4Ti3O12 and TiO2 coated Bi4Ti3O12 nanoparticles is shown in Figure 1. The samples exhibit well-crystallized perovskite phase of Bi4Ti3O12 according to the JCPDS database card number 47-0398. The average particle size calculated is around 56 nm by Scherrer formula. There was no diffraction peak for TiO2 after the coating process.Figure 1
X-ray diffraction pattern of Bi4Ti3O12- and TiO2-coated Bi4Ti3O12 nanoparticles annealed at 690°C for 2 h.Figure2 shows the surface morphology image of the Bi4Ti3O12 film (a) and TiO2 coated Bi4Ti3O12 (b) in top views. It can be seen that the Bi4Ti3O12 film grown on FTO substrates possesses a high degree of porosity which was the key factor to obtain efficient dye-sensitized solar cells. The size of the nanoparticles is in the range of 100–200 nm which is much larger than the XRD result. The thickness of the Bi4Ti3O12 film is about 15 μm. After the modification, most of the Bi4Ti3O12 nanoparticles were coated with TiO2.SEM micrographs the thin film. (a) Bi4Ti3O12 top view, (b) TiO2 coated Bi4Ti3O12.
(a)(b)


### 3.2. UV-vis Absorption Spectra

The UV-vis absorption spectra of N3 dye in ethanol solution (curve a), Bi4Ti3O12 nanoparticles (curve b), and N3-sensitized Bi4Ti3O12 nanoparticles (curve c) are illustrated in Figure 3. The spectrum (curve b) of Bi4Ti3O12 nanoparticles exhibits a typical optical absorption behavior of a wide-band gap semiconducting oxide, having an intense absorption band with a steep edge. When N3 dye molecules are adsorbed onto the surface of the Bi4Ti3O12 nanoparticles, a new absorption band around 524 nm emerges in the visible region (curve c) compared with that of bare Bi4Ti3O12 nanoparticles (curve b) which evidently originates from the absorption of dye molecules. However, the maximum absorption at 500 nm of pure N3 dye is shifted to 524 nm. The red shift might be attributed to the interaction between the dye molecules and semiconductor surface which shows the potential application in dye-sensitized solar cells [21–23].Figure 3
UV-vis absorption spectra of N3 (curve a), Bi4Ti3O12 nanoparticles (curve b), and N3 sensitized Bi4Ti3O12 nanoparticles (curve c).


### 3.3. Surface Photovoltage Spectroscopy Analysis

In our previous work, it has been found that the Bi4Ti3O12 thin compact film exhibited obvious surface photovoltaic response, which is attributed to the electronic transition from the O 2p valence band to the Ti 3d conduction band. Figure 4 shows the SPS spectra of bare and N3 sensitized Bi4Ti3O12 nanoparticles. The surface photovoltaic response of the bare Bi4Ti3O12 nanoparticles appeared in the wavelength range of 310–420 nm with a maximum at 361 nm. After the absorption of N3, a new SPS response band emerges in the visible region of 420–600 nm, which extends the onset of the surface photovoltaic response of Bi4Ti3O12 from 420 to 600 nm. The clear SPV peak indicates that photo-induced electron-hole pairs are easily and effectively separated on the basis of the SPS principle in the visible light.Figure 4
SPS spectra of Bi4Ti3O12 nanoparticles (curve a) and N3-sensitized Bi4Ti3O12 nanoparticles (curve b).


### 3.4. Performance of DSSCs

Based on the previous study, application of Bi4Ti3O12 film in dye-sensitized solar cells seems to be possible. However, the adsorption of dye on Bi4Ti3O12 film is slow. In this study, all the photoelectrode was soaked in the dye ethanol solution at least for 48 h to achieve better dye adsorption. Figure 5 shows the J-V characteristics of the DSC based on pure Bi4Ti3O12, pure TiO2, and TiO2-modified Bi4Ti3O12 nanoporous electrodes. It can be seen that the photoelectrical performance of Bi4Ti3O12 is similar with the simple binary oxides, such as TiO2 and ZnO. But the overall light to electricity conversion efficiency is as low as 0.02%. The factors which contribute to the conversion efficiency are short-circuit current (JSC), open-circuit voltage (VOC), and the fill factor (FF). The three main parameters are 0.13 mA cm−2, 0.38 V, and 0.40, respectively (shown in Table 1.).Table 1
Photoelectrochemical parameters of DSSCs using bare and 5 at % TiO2-modified Bi4Ti3O12 nanoporous electrodes.
SampleJSC /mA cm−2VOC /mVffη/%Bare Bi4Ti3O12/N30.130.380.400.02TiO2/N31.640.650.500.53Bi4Ti3O12/TiO2/N30.970.720.690.48Figure 5
J-V characteristics of bare (curve a) and 5 at % TiO2-modified Bi4Ti3O12 (curve b) thin films.To improve the photoelectrical performance of Bi4Ti3O12 electrode, the efficient way is coating the photoelectrode with other semiconducting oxide, such as Al2O3, ZnO, and so on [4, 24]. Here, we modified the Bi4Ti3O12 film with TiO2 by addition of 5% (a.t.) tetrabutyl titanate to the colloid of Bi4Ti3O12 in 1-butanol before the doctor blading process. Remarkable improvements were found in every aspect of short-circuit current (JSC), open-circuit voltage (VOC), and the fill factor (ff) (shown in Table 1.). The JSC was improved by nearly seven times. The VOC and fill factor also showed an improvement of 340 mV and 0.29. The overall efficiency reached 0.48%. The Property of the pure TiO2 electrode prepared by the doctor blading of the 1-butanol solution of tetrabutyl titanate was also given in Figure 5. It can be seen that the TiO2 modified Bi4Ti3O12 also shows higher open circuit voltage than the pure TiO2 electrode. To explore the causes for the enhancement of the photoelectrochemical properties of DSCs, the dye absorption, flat band potential, and dark current were investigated.The restriction of charge recombination at the semiconductor/dye/electrolyte interface is an efficient method for the improvement ofVOC and FF of DSSCs [25, 26]. The dark current arises from the reduction of triiodide and oxidized dye molecule by conduction band electrons of semiconductor films [25, 26]. The dark current measurement is an apparent analysis on the interface charge recombination. Figure 6 addresses the dark current for the dye-sensitized solar cells using pure Bi4Ti3O12, pure TiO2, and TiO2-modified Bi4Ti3O12 nanoporous electrodes. The TiO2-modified Bi4Ti3O12 shows lower recombination than pure Bi4Ti3O12, and pure TiO2 which contributes to the elevation of VOC and fill factor.Figure 6
Dark current characteristics of bare (curve a) and 5 at % TiO2-modified Bi4Ti3O12 (curve b) thin films.The flat band potential (Vfb) of pure Bi4Ti3O12, pure TiO2, and TiO2 coated Bi4Ti3O12 electrode were evaluated through the Mott-Schottky analysis method. This analysis method is based on the capacitance versus applied potential measurement. The relationship between the capacitance and the applied potential can be expressed by the following equation:(1)1CSC2=2(|V-Vfb|-kT/e)εε0eND,
[27]where CSC is the space-charge capacitance, ε is the dielectric constant of the semiconductor, ε0 is the permittivity of free space, ND is the dopant density, Vfb is the flat band potential, and Vis the applied potential. Figure 7 shows the Mott-Schottky curves of pure Bi4Ti3O12, pure TiO2, and TiO2 coated Bi4Ti3O12 films. The plot of CSC-2 versus polarization potential shows an X-intercept corresponding to Vfb. The flat band potential of pure Bi4Ti3O12 and pure TiO2 was determined to be about −0.58 V and −0.47 V (versus Ag/AgCl). But the Vfb of TiO2 coated Bi4Ti3O12 shifts significantly toward the cathodic potential which should cause the improvement of open-circuit voltage (VOC) [27, 28].Figure 7
Mott-Schottky plots of bare (curve a) and 5 at % TiO2-modified Bi4Ti3O12 (curve b) thin films, Vfb, the flat band potential.The amount of dye absorption is one of the important factors on the short-circuit current of DSSCs. The dye absorbed on Bi4Ti3O12 electrode is about 1.4E-8 mol cm−2 which contributes to the low photocurrent. However, no significant change was found in our study before and after TiO2 coating on the Bi4Ti3O12 films. So other controlling process should exist, such as the electron transfer process from excited dye molecular to the conduction band of Bi4Ti3O12 and the electron transport process in the Bi4Ti3O12 film. Though the overall efficiency of Bi4Ti3O12 is severely lower than that of TiO2, there are many ways to ameliorate the performance for this multication oxide, the variation of the relative Bi/Ti ratio, the partial replacement of Bi or Ti by other metal ion. From this work we can conclude that Bi4Ti3O12 film is a potential photoanode material for DSSCs.


## 3.1. Structures and Morphologies

The XRD pattern of the as-prepared Bi4Ti3O12 and TiO2 coated Bi4Ti3O12 nanoparticles is shown in Figure 1. The samples exhibit well-crystallized perovskite phase of Bi4Ti3O12 according to the JCPDS database card number 47-0398. The average particle size calculated is around 56 nm by Scherrer formula. There was no diffraction peak for TiO2 after the coating process.Figure 1
X-ray diffraction pattern of Bi4Ti3O12- and TiO2-coated Bi4Ti3O12 nanoparticles annealed at 690°C for 2 h.Figure2 shows the surface morphology image of the Bi4Ti3O12 film (a) and TiO2 coated Bi4Ti3O12 (b) in top views. It can be seen that the Bi4Ti3O12 film grown on FTO substrates possesses a high degree of porosity which was the key factor to obtain efficient dye-sensitized solar cells. The size of the nanoparticles is in the range of 100–200 nm which is much larger than the XRD result. The thickness of the Bi4Ti3O12 film is about 15 μm. After the modification, most of the Bi4Ti3O12 nanoparticles were coated with TiO2.SEM micrographs the thin film. (a) Bi4Ti3O12 top view, (b) TiO2 coated Bi4Ti3O12.
(a)(b)


## 3.2. UV-vis Absorption Spectra

The UV-vis absorption spectra of N3 dye in ethanol solution (curve a), Bi4Ti3O12 nanoparticles (curve b), and N3-sensitized Bi4Ti3O12 nanoparticles (curve c) are illustrated in Figure 3. The spectrum (curve b) of Bi4Ti3O12 nanoparticles exhibits a typical optical absorption behavior of a wide-band gap semiconducting oxide, having an intense absorption band with a steep edge. When N3 dye molecules are adsorbed onto the surface of the Bi4Ti3O12 nanoparticles, a new absorption band around 524 nm emerges in the visible region (curve c) compared with that of bare Bi4Ti3O12 nanoparticles (curve b) which evidently originates from the absorption of dye molecules. However, the maximum absorption at 500 nm of pure N3 dye is shifted to 524 nm. The red shift might be attributed to the interaction between the dye molecules and semiconductor surface which shows the potential application in dye-sensitized solar cells [21–23].Figure 3
UV-vis absorption spectra of N3 (curve a), Bi4Ti3O12 nanoparticles (curve b), and N3 sensitized Bi4Ti3O12 nanoparticles (curve c).


## 3.3. Surface Photovoltage Spectroscopy Analysis

In our previous work, it has been found that the Bi4Ti3O12 thin compact film exhibited obvious surface photovoltaic response, which is attributed to the electronic transition from the O 2p valence band to the Ti 3d conduction band. Figure 4 shows the SPS spectra of bare and N3 sensitized Bi4Ti3O12 nanoparticles. The surface photovoltaic response of the bare Bi4Ti3O12 nanoparticles appeared in the wavelength range of 310–420 nm with a maximum at 361 nm. After the absorption of N3, a new SPS response band emerges in the visible region of 420–600 nm, which extends the onset of the surface photovoltaic response of Bi4Ti3O12 from 420 to 600 nm. The clear SPV peak indicates that photo-induced electron-hole pairs are easily and effectively separated on the basis of the SPS principle in the visible light.Figure 4
SPS spectra of Bi4Ti3O12 nanoparticles (curve a) and N3-sensitized Bi4Ti3O12 nanoparticles (curve b).


## 3.4. Performance of DSSCs

Based on the previous study, application of Bi4Ti3O12 film in dye-sensitized solar cells seems to be possible. However, the adsorption of dye on Bi4Ti3O12 film is slow. In this study, all the photoelectrode was soaked in the dye ethanol solution at least for 48 h to achieve better dye adsorption. Figure 5 shows the J-V characteristics of the DSC based on pure Bi4Ti3O12, pure TiO2, and TiO2-modified Bi4Ti3O12 nanoporous electrodes. It can be seen that the photoelectrical performance of Bi4Ti3O12 is similar with the simple binary oxides, such as TiO2 and ZnO. But the overall light to electricity conversion efficiency is as low as 0.02%. The factors which contribute to the conversion efficiency are short-circuit current (JSC), open-circuit voltage (VOC), and the fill factor (FF). The three main parameters are 0.13 mA cm−2, 0.38 V, and 0.40, respectively (shown in Table 1.).Table 1
Photoelectrochemical parameters of DSSCs using bare and 5 at % TiO2-modified Bi4Ti3O12 nanoporous electrodes.
SampleJSC /mA cm−2VOC /mVffη/%Bare Bi4Ti3O12/N30.130.380.400.02TiO2/N31.640.650.500.53Bi4Ti3O12/TiO2/N30.970.720.690.48Figure 5
J-V characteristics of bare (curve a) and 5 at % TiO2-modified Bi4Ti3O12 (curve b) thin films.To improve the photoelectrical performance of Bi4Ti3O12 electrode, the efficient way is coating the photoelectrode with other semiconducting oxide, such as Al2O3, ZnO, and so on [4, 24]. Here, we modified the Bi4Ti3O12 film with TiO2 by addition of 5% (a.t.) tetrabutyl titanate to the colloid of Bi4Ti3O12 in 1-butanol before the doctor blading process. Remarkable improvements were found in every aspect of short-circuit current (JSC), open-circuit voltage (VOC), and the fill factor (ff) (shown in Table 1.). The JSC was improved by nearly seven times. The VOC and fill factor also showed an improvement of 340 mV and 0.29. The overall efficiency reached 0.48%. The Property of the pure TiO2 electrode prepared by the doctor blading of the 1-butanol solution of tetrabutyl titanate was also given in Figure 5. It can be seen that the TiO2 modified Bi4Ti3O12 also shows higher open circuit voltage than the pure TiO2 electrode. To explore the causes for the enhancement of the photoelectrochemical properties of DSCs, the dye absorption, flat band potential, and dark current were investigated.The restriction of charge recombination at the semiconductor/dye/electrolyte interface is an efficient method for the improvement ofVOC and FF of DSSCs [25, 26]. The dark current arises from the reduction of triiodide and oxidized dye molecule by conduction band electrons of semiconductor films [25, 26]. The dark current measurement is an apparent analysis on the interface charge recombination. Figure 6 addresses the dark current for the dye-sensitized solar cells using pure Bi4Ti3O12, pure TiO2, and TiO2-modified Bi4Ti3O12 nanoporous electrodes. The TiO2-modified Bi4Ti3O12 shows lower recombination than pure Bi4Ti3O12, and pure TiO2 which contributes to the elevation of VOC and fill factor.Figure 6
Dark current characteristics of bare (curve a) and 5 at % TiO2-modified Bi4Ti3O12 (curve b) thin films.The flat band potential (Vfb) of pure Bi4Ti3O12, pure TiO2, and TiO2 coated Bi4Ti3O12 electrode were evaluated through the Mott-Schottky analysis method. This analysis method is based on the capacitance versus applied potential measurement. The relationship between the capacitance and the applied potential can be expressed by the following equation:(1)1CSC2=2(|V-Vfb|-kT/e)εε0eND,
[27]where CSC is the space-charge capacitance, ε is the dielectric constant of the semiconductor, ε0 is the permittivity of free space, ND is the dopant density, Vfb is the flat band potential, and Vis the applied potential. Figure 7 shows the Mott-Schottky curves of pure Bi4Ti3O12, pure TiO2, and TiO2 coated Bi4Ti3O12 films. The plot of CSC-2 versus polarization potential shows an X-intercept corresponding to Vfb. The flat band potential of pure Bi4Ti3O12 and pure TiO2 was determined to be about −0.58 V and −0.47 V (versus Ag/AgCl). But the Vfb of TiO2 coated Bi4Ti3O12 shifts significantly toward the cathodic potential which should cause the improvement of open-circuit voltage (VOC) [27, 28].Figure 7
Mott-Schottky plots of bare (curve a) and 5 at % TiO2-modified Bi4Ti3O12 (curve b) thin films, Vfb, the flat band potential.The amount of dye absorption is one of the important factors on the short-circuit current of DSSCs. The dye absorbed on Bi4Ti3O12 electrode is about 1.4E-8 mol cm−2 which contributes to the low photocurrent. However, no significant change was found in our study before and after TiO2 coating on the Bi4Ti3O12 films. So other controlling process should exist, such as the electron transfer process from excited dye molecular to the conduction band of Bi4Ti3O12 and the electron transport process in the Bi4Ti3O12 film. Though the overall efficiency of Bi4Ti3O12 is severely lower than that of TiO2, there are many ways to ameliorate the performance for this multication oxide, the variation of the relative Bi/Ti ratio, the partial replacement of Bi or Ti by other metal ion. From this work we can conclude that Bi4Ti3O12 film is a potential photoanode material for DSSCs.


## 4. Conclusions

In conclusion, Bi4Ti3O12 film could be efficiently sensitized with N3 dye. The sensitized Bi4Ti3O12 film shows significant absorbance and surface photovoltaic response in visible light which indicates the emergence of chemical interaction between the dye molecules and semiconductor surface. This ternary oxide exhibited similar photoelectrical performance with TiO2. But poor performance was obtained because of the severe charge recombination and lower conduction band edge. After TiO2 modification, the three main parameters short-circuit current (JSC), open-circuit voltage (VOC), and the fill factor (FF) are 0.97 mA cm−2, 0.72 V, and 0.69, respectively. The overall efficiency reached 0.48%. Potential improvement can be anticipated by the decrease of the particle size and optimization of the compositions.



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*Source: 821045-2011-08-17.xml*