# Effect of Silver Nanoparticle Size on Efficiency Enhancement of Dye-Sensitized Solar Cells

Authors: Chanu Photiphitak; Pattana Rakkwamsuk; Pennapa Muthitamongkol; Chaiyuth Sae-Kung; Chanchana  Thanachayanont
Journal: International Journal of Photoenergy
 (2011)

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## Abstract

Titanium dioxide/silver (TiO2/Ag) composite films were prepared by incorporating Ag in pores of mesoporous TiO2 films using a photoreduction method. The Ag nanoparticle sizes were in a range of 4.36–38.56 nm. The TiO2/Ag composite films were characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM) and transmission electron microscopy (TEM). The TiO2 and TiO2/Ag composite films were then sensitized by immersing in a 0.3 mM N719 dye solution and fabricated for conventional dye-sensitized solar cells (DSCs). J-V characteristics of the TiO2/Ag DSCs showed that the Ag nanoparticle size of 19.16 nm resulted in the short circuit current density and efficiency of 8.12 mA/cm2 and 4.76%.


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## Body

## 1. Introduction

Surface plasmon resonance induced by silver (Ag) nanoparticles leads to an increase in an absorption coefficient of dye in dye-sensitized solar cells (DSCs) [1–6]. The effect has been theoretically described as an increase of local electromagnetic field nearby metal surfaces which is found when wavelengths of irradiation sources are correlated with the optical absorption of the surface plasmon resonance [7–11]. The modification of the surfaces for an enhancement of optical absorption, hence, provides a good method to improve efficiency of an optoelectronic device involving photon absorption [12]. Several methods for the fabrication of the silver nanoparticles were studied such as thermal evaporation of Ag islands on titanium dioxide (TiO2) films [1], magnetron sputtering of TiO2 and Ag composite films [13], electrochemical deposition of Ag by double pulse method on indium tin oxide (ITO) [14], loading of Ag and silver chloride (AgCl) onto anatase TiO2 nanotubes that were grown by a hydrothermal treatment [15] and loading of the Ag nanoparticles onto self-organized TiO2 nanotube layers using photocatalytic reduction  [16, 17].Wen et al. [1] generated the Ag island films by depositing the 3.3–6.0 nm-thick Ag nanoparticle layer on the TiO2 film electrode using thermal evaporation and found a possibility of using plasmon resonance effect to enhance the efficiency of the DSCs, if the volume and structure of the Ag island films could be controlled and optimized. Ihara et al. [18] improved photoelectric conversion efficiency of their dye-sensitized solar cells by using localized surface plasmon of the Ag nanoparticles (diameter of 12.5 nm) modified with polymer and reported that the efficiency of dye-sensitized solar cell with the Ag nanoparticles increased from 1.5% to 2.5%  compared with the case with no Ag nanoparticles. Chen et al. [19] studied effects of adding silver nanowires (40 nm in diameter and 20 μm in length) in the anode of the DSCs to improve the photovoltaic efficiency. Results showed that the composite anode of Ag nanowires and TiO2/P25 has improved photovoltaic conversion efficiency about two times of standard P-25 DSCs. Chou et al. [20] prepared TiO2/Ag composite particles by dry particle-coating technique. The Ag particle size was bigger than 100 nm, and the TiO2/Ag composite particles were found to improve the efficiency of the DSCs because Schottky barrier exceeded that of the conventional DSCs.In this study, for a cost-effective process, we prepared the Ag nanoparticles with sizes in a range of 4.36–38.56 nm using a photoreduction method. The Ag nanoparticles were deposited onto the mesoporous anatase TiO2 electrode with worm-like pores. The Ag nanoparticles were incorporated thoroughly into the pores of the mesoporous TiO2 film electrode [21–24]. The effect of the Ag nanoparticle size on the efficiency enhancement of dye-sensitized solar cells was investigated. The optimum DSC in this study showed a maximum efficiency of 4.76%. Although the 5.45% efficiency by using a similar material (TiO2/Ag/DSC) has been showed in 2007 by Ramasamy et al. [25], this is the first time that the effect of Ag particle sizes is carefully investigated.


## 2. Materials and Methods

### 2.1. The Preparation of Mesoporous TiO2 Electrodes

The TiO2 electrodes were screen printed from a TiO2 paste (Dyesol) 3 times on a fluorine-doped tin oxide (FTO) glass substrate (2×3 cm2 in size). A 200 mesh was used to obtain a TiO2 layer with area of 0.5×1.2 cm2 and a thickness of approximately 13.8 μm (see Figure 1). In order to avoid contamination on the fresh film, screen printing was performed in a clean-room environment. After drying at 55°C for 30 minutes, the electrodes were sintered at 450°C for 30 minutes, and then cooled down to room temperature. The electrodes were immersed in a 3×10-4 M of N719 dye solution, namely, cis-diisothiocyanato-bis(2,2-bipyridyl-4,4- dicarboxylatoe) ruthenium (II)bis (tetrabutylammonium) in absolute ethanol for 24 hours. The excess dye was removed from the electrode by rinsing with ethanol.Figure 1
An SEM image showing a cross-section of the TiO2 film.


### 2.2. The Synthesis of Mesoporous TiO2/Ag Films

In order to deposit the Ag nanoparticles on the TiO2 film, a 2×3 cm2 FTO glass with 0.5×1.2 cm2 TiO2 films was immersed in the 0.1 M AgNO3 solution for five seconds, then rinsed with DI water and dried in a N2 stream. The films were then exposed to a UV irradiation at λ=254 nm using a Spectroline CM-10 Fluorescence Analysis Cabinet at an intensity of ~0.31 mW/cm2. We designed the experiment to vary exposure times for 5, 10, 15, 20, 30, 60, 90, 120, 150, 180, and 240 minutes for the photocatalytic reduction of Ag+ to the metallic Ag nanoparticles. Finally, the TiO2/Ag electrodes were immersed in dye solution for 24 hours and prepared for dye-sensitized solar cells.


### 2.3. The Preparation of Pt Counter Electrodes

The counter electrodes were prepared by screen printing a thin layer of platinum (Pt) with a size of0.5×1.2 cm2 using a platinum paste (Dyesol), on an FTO glass substrate (2×3 cm2), and then sintered at 450°C for 30 minutes.


### 2.4. DSC Fabrication

A sandwich-type cell [26] was fabricated by assembling a sensitized TiO2 electrode using surlyn-based polymer sheet (80 μm thick) and sealed by a hot gun for a few seconds.  The liquid electrolyte contained 0.5 M LiI, 0.05 M I2, and 0.5 M 4-tert-butyl pyridine in 90 : 10 v/v of acetonitrile: 3 methyl-2-oxazolidinone. Electrolyte-injecting holes, made on the counter-electrode side, were sealed with surlyn and glass cover.


### 2.5. Measurements

Optical absorption spectra of the film electrode samples were measured using a UV-visible spectrophotometer (Jasco model: V-530). In order to observe the microstructure and elemental analysis of the obtained Ag nanoparticles, the Ag nanoparticles were prepared on carbon-coated copper grids for observations by transmission electron microscopy (TEM JEOL model JSM-2010). The X-ray diffraction (XRD JEOL-300) patterns were obtained by analyzing the Ag/TiO2 films on the glass substrates. Scanning electron microscope (SEM JEOL model: JSM-6301 F)  was employed to record cross-sectional micrographs of the Ag/TiO2 films. J-V measurements were performed under a 450 W xenon light source which is able to provide 1000 W·m−2 sunlight equivalent irradiation (AM 1.5), using Keithley digital source meter (Model 2400) under the illuminated condition.


## 2.1. The Preparation of Mesoporous TiO2 Electrodes

The TiO2 electrodes were screen printed from a TiO2 paste (Dyesol) 3 times on a fluorine-doped tin oxide (FTO) glass substrate (2×3 cm2 in size). A 200 mesh was used to obtain a TiO2 layer with area of 0.5×1.2 cm2 and a thickness of approximately 13.8 μm (see Figure 1). In order to avoid contamination on the fresh film, screen printing was performed in a clean-room environment. After drying at 55°C for 30 minutes, the electrodes were sintered at 450°C for 30 minutes, and then cooled down to room temperature. The electrodes were immersed in a 3×10-4 M of N719 dye solution, namely, cis-diisothiocyanato-bis(2,2-bipyridyl-4,4- dicarboxylatoe) ruthenium (II)bis (tetrabutylammonium) in absolute ethanol for 24 hours. The excess dye was removed from the electrode by rinsing with ethanol.Figure 1
An SEM image showing a cross-section of the TiO2 film.


## 2.2. The Synthesis of Mesoporous TiO2/Ag Films

In order to deposit the Ag nanoparticles on the TiO2 film, a 2×3 cm2 FTO glass with 0.5×1.2 cm2 TiO2 films was immersed in the 0.1 M AgNO3 solution for five seconds, then rinsed with DI water and dried in a N2 stream. The films were then exposed to a UV irradiation at λ=254 nm using a Spectroline CM-10 Fluorescence Analysis Cabinet at an intensity of ~0.31 mW/cm2. We designed the experiment to vary exposure times for 5, 10, 15, 20, 30, 60, 90, 120, 150, 180, and 240 minutes for the photocatalytic reduction of Ag+ to the metallic Ag nanoparticles. Finally, the TiO2/Ag electrodes were immersed in dye solution for 24 hours and prepared for dye-sensitized solar cells.


## 2.3. The Preparation of Pt Counter Electrodes

The counter electrodes were prepared by screen printing a thin layer of platinum (Pt) with a size of0.5×1.2 cm2 using a platinum paste (Dyesol), on an FTO glass substrate (2×3 cm2), and then sintered at 450°C for 30 minutes.


## 2.4. DSC Fabrication

A sandwich-type cell [26] was fabricated by assembling a sensitized TiO2 electrode using surlyn-based polymer sheet (80 μm thick) and sealed by a hot gun for a few seconds.  The liquid electrolyte contained 0.5 M LiI, 0.05 M I2, and 0.5 M 4-tert-butyl pyridine in 90 : 10 v/v of acetonitrile: 3 methyl-2-oxazolidinone. Electrolyte-injecting holes, made on the counter-electrode side, were sealed with surlyn and glass cover.


## 2.5. Measurements

Optical absorption spectra of the film electrode samples were measured using a UV-visible spectrophotometer (Jasco model: V-530). In order to observe the microstructure and elemental analysis of the obtained Ag nanoparticles, the Ag nanoparticles were prepared on carbon-coated copper grids for observations by transmission electron microscopy (TEM JEOL model JSM-2010). The X-ray diffraction (XRD JEOL-300) patterns were obtained by analyzing the Ag/TiO2 films on the glass substrates. Scanning electron microscope (SEM JEOL model: JSM-6301 F)  was employed to record cross-sectional micrographs of the Ag/TiO2 films. J-V measurements were performed under a 450 W xenon light source which is able to provide 1000 W·m−2 sunlight equivalent irradiation (AM 1.5), using Keithley digital source meter (Model 2400) under the illuminated condition.


## 3. Results and Discussion

### 3.1. Morphology of the TiO2/Ag Deposited Films

The TiO2 films were prepared by screen printing 3 layers of the TiO2 paste and calcination at 450°C for 30 minutes. A thickness measured using SEM is approximately 13.8 μm as shown in Figure 1 (in agreement with [27–30]).The TiO2 films were loaded with the Ag nanoparticles using the AgNO3 soaking and the UV illumination treatment described in the experimental part 2.2. After the films were irradiated by the UV light, they turned brownish grey in a few minutes due to photocatalytic reduction of Ag+ to Ag [31]. The Ag nanoparticles on the TiO2 particles were not readily observed by the SEM (Figure 2). However, The TiO2/Ag composite films were characterized using energy dispersive X-Ray spectroscopy (EDX) technique attached to the SEM. We found that the peaks of the Ag nanoparticles were present (Figure 2), suggesting the presence of the Ag nanoparticles on surface of the TiO2 films.Figure 2
An SEM cross-sectional micrograph of the TiO2/Ag composite film with a UV exposure for 120 minutes. Inset shows an EDX spectrum indicating the presence of the Ag nanoparticles on the TiO2 films.Figure3(a) shows a TEM micrograph of the TiO2 nanoparticles from the TiO2 films before immersion in the AgNO3 solution. We found that the TiO2 nanoparticles were nanorods and the lengths were approximately 25 nm. Figure 3(b) shows an example of the TEM images of the TiO2 nanorods from the films after immersion in the AgNO3 solution and exposed to the UV irradiation for 120 minutes. The result shows the presence of the TiO2 nanorods and the spherical Ag nanoparticles adsorbed on surfaces of the TiO2 nanorods. An example of XRD pattern of the TiO2/Ag composite films (Figure 4) shows that four 2θ diffraction peaks at 38.12, 44.30, 64.44, and 77.40 could, respectively, be indexed as (111), (200), (220), and (311) planes of face-centered cubic Ag. Peaks at 25.36, 37.05, 37.90, 48.15, and 54.05 are indexed as (101), (103), (004), (200), and (105) planes of the anatase TiO2.TEM micrographs of the TiO2 nanotubes  (a) before and (b) after immersion in the AgNO3 solution with UV exposure for  120 minutes.
(a)(b)Figure 4
XRD peaks of the TiO2/Ag composite film with UV exposure for 120 minutes on an FTO glass substrate. (Note: graph plotted by OriginLab software program.)The Ag nanoparticles were also prepared on the carbon-coated copper grids and exposed to varied UV exposure times of 0, 5, 10, 15, 20, 30, 60, 90, 120, 150, 180 and 240 minutes. The average diameters of the Ag nanoparticles measured from the TEM micrographs using Image-Pro Plus 5.0 software program were approximately4.36±2.53, 4.56±1.78, 5.39±1.83, 6.20±1.65, 7.17±2.59, 10.98±1.80, 15.57±3.26, 19.16±3.71, 23.55±4.26, 27.51±8.05, and  38.56±5.30, respectively. The sizes of Ag nanoparticles were found to depend strongly on the UV exposure time (Figure 5) due to the photocatalytic reduction of the Ag+ to the Ag metal in the form of the Ag nanoparticles where electrons were provided by water [17, 31].TEM micrographs and size distributions of silver nanoparticles prepared by photocatalytic reduction in a 0.1 M AgNO3 solution on the carbon-coated copper grids at UV exposure times of (a) 5 minutes, (b) 120 minutes, and (c) 240 minutes, respectively. The average size increases and the distribution broadens with an increase in the UV exposure time. (Note: graph plotted by OriginLab software program).
(a)(b)(c)


### 3.2. The Effect of the Ag Nanoparticle Size on Optical Absorption Spectra

The absorption spectrum of the Ag nanoparticles exhibits the surface plasmon peak at approximately 400 nm on the broad band [32]. Optical absorption spectra can be theoretically calculated using Mie's theory. When the particles having diameter (R) are suspended in a medium with the dielectric constant (εm), the dipolar absorption efficiency (Qabs) is given by(1)Qabs=24πRλ⋅εm3/2ε′′(ω)ε′′(ω)2+〈ε′(ω)+2εm+48π2R2εm2/5λ2〉2,
where λ is a wavelength of the incoming light in the medium, and ε′(ω) and ε′′(ω) represent the real and imaginary parts of the dielectric function, ε(ω), respectively, [ε(ω)=ε′(ω)+ε′′(ω)].  Thus, the absorption efficiency of particles is a function of the dielectric constant of the metal, that of medium and the size of the particle.From (1), the Mie's theory only successfully explains the absorption band for metallic nanoparticles in visible range, and,for radius less than 5 nm, the width of the surface plasmon peak increases linearly with the reciprocal of the radius [32, 33]. On the other hand, the width of the surface plasmon peak increases with an increase in the radius in the range larger than 10 nm, because of inhomogeneous polarization of the particles in the electromagnetic field of the incoming light due to excitation of a different multiple modes which makes a peak in the spectrum at a different energy [32, 34]. Figure 6(a) shows optical absorption spectra of the Ag nanoparticles films indicating an increase in wavelength (red shifted) with an increase in the diameters of the Ag nanoparticles because the width of the surface plasmon peak increases.Optical absorption spectra of: (a) the Ag nanoparticle films with various particle sizes of the Ag nanoparticles in the range of 4.36–38.56 nm and (b) the Ag/N719 dye film compared with an optical absorption spectrum of3×10-5 M N719 dye solution.
(a)(b)Figure6(b) shows the absorption peak of the Ag/N719 dye film, it is found that the Ag 19.16 nm/N719dye film has a maximum peak width or red shift due to the surface plasmon resonance of the silver particles contributing to the absorption coefficient of the dye. The absorption of the Ru-dye can occur via the metal-ligand charge-transfer transition (MLCT), t2→π* MLCT transitions in the absorption maximum at 396 and 534 nm, and π→π* intraligand transition in the UV [35]. Thus, both the surface Plasmon resonance absorption of Ag nanoparticles and the Ru-dye absorption for MLCT transition contributed to the total absorption.


### 3.3. The Effect of the Ag Nanoparticle Size on Efficiency of the DSCs

Parameters extracted fromJ-V characteristics, for example, Figure 8, of the TiO2/Ag composite film electrode DSCs are shown in Table 1. The Ag nanoparticles of the average size of 19.16 nm (3.59±0.50 weight % of Ag nanoparticles in the TiO2/Ag composite) were found to result in the maximum value of short circuit current density of 8.12 mA/cm2.Table 1
Weight (%) of Ag nanoparticles obtained from SEM-EDX analysis, short circuit current densities (JSC), open circuit voltages (VOC), fill factors (FF), and efficiencies of DSCs prepared using the TiO2/Ag composite film electrodes compared with pure TiO2 electrode (reference) under AM1.5.
No.Size of Agnanoparticles on TiO2 electrode (nm)Weight (%) of Ag nanoparticlesJSC (mA/cm2)VOC (V)FFEfficiency (%)1pure TiO2 (reference)07.500.720.754.0224.36±2.533.30±0.357.070.750.764.0234.56±1.784.01±0.568.110.740.684.0745.39±1.833.52±0.277.210.760.623.4056.20±1.653.45±0.307.840.740.623.6467.17±2.593.56±0.306.810.780.633.34710.98±1.803.54±0.386.320.770.783.82812.5 [18]—4.400.810.692.5915.57±3.263.29±0.116.810.750.783.981019.16±3.713.59±0.508.120.730.804.761123.55±4.264.14±0.946.430.760.753.641227.51±8.054.20±0.346.040.760.763.511338.56±5.304.42±0.456.190.740.753.431440 [19]—11.530.650.534.1015~100 [20]—2.100.820.540.93As shown in Table1, the pure TiO2 electrode (reference cell) results in the short circuit current density (JSC) of 7.50 mA/cm2, open circuit voltages (VOC) of 0.72 V, fill factors (FF) of 0.75, and efficiency of 4.02%. For the TiO2/Ag electrodes, after improvement with intercalation of Ag nanoparticles of which size ranging from 4.36 to 38.56 nm, we found that the dye-sensitized solar cell which was prepared from the TiO2/Ag (19.16 nm) electrode had maximum values of the JSC, FF, and efficiency of 8.12 mA/cm2, 0.80 and 4.76%, respectively, with VOC of 0.73. Compared with the reference cell, the TiO2/Ag (19.16 nm) is found to improve JSC, FF, and efficiency because of an optimum electromagnetic field introduced by the silver plasmon resonance that enhances the optical absorption of the dye [2, 3, 36]. The other possible reason is that the Ag nanoparticles have a catalytic effect that increases the reaction rate between the semiconductor, dye, and the redox electrolyte and/or the internal photoemission from the Ag nanoparticles increases the photocurrent [1, 3, 36]. However, the dye-sensitized solar cells which were prepared from the TiO2/Ag electrodes with the Ag nanoparticle sizes bigger than 19.16 nm have low values of the JSC. It is believed that with the Ag particle sizes bigger than 19.16 nm, Schottky barriers formed at the TiO2/Ag contacts become dominant and retard electron transport in the conduction bands [1, 3, 37, 38].Figure7 plots JSC, VOC, FF, and efficiencies versus the sizes of the Ag nanoparticles. The DSCs in our study were compared with the Ag nanoparticle size of around 12.5 [18], 40 [19], and 100 [20] nm on the TiO2 electrodes reported elsewhere. Due to different thicknesses of the TiO2 layers prepared, direct comparison cannot be made. However, the improved JSC of the best DSC prepared in this study is noteworthy. Compared with the reported DSCs with the Ag nanowires of 40 nm in diameter and 20 μm in length [19] with the JSC of 11.53 mA/cm2, the best DSC in this study has a lower value of JSC. The high value of JSC in the Ag nanowire DSCs has been reported to be due to metal network formation by adding Ag nanowires to improve the production and transportation of photon-generated current [39].Figure 7
Open circuit voltages (VOC), short circuit current densities (JSC), fill factors (FF), and efficiencies of the DSCs  with varied sizes of the Ag nanoparticles compared with reported  DSCs [18–20]. At [18], use 2 μm of TiO2 thickness and size of 0.25 cm2, [19] use 15 μm of TiO2 thickness and size of 0.25 cm2, [20] use 8.1 μm of TiO2 thickness and size of 4.0 cm2, and this study uses 13.8 μm of TiO2 thickness and size of 0.6 cm2.Figure 8
J-V characteristics of the DSCs composed of the TiO2 electrodes with N719 dye before and after improvement with the Ag nanoparticles.However theVOC, FF, and efficiency values of the Ag nanowire DSCs are not higher than the best value reported in this study. When compared with the reported DSCs with the Ag nanoparticle size of around 100 nm [20], the values of JSC, VOC, FF and Efficiency follow a decreasing trend after the maximum values because the Schottky barriers formed at the TiO2/Ag contact retarding electron transport in conduction bands [1, 3]. Therefore, the Ag nanoparticles size of 19.16 nm prepared in this study is an appropriate size to improve JSC of the DSCs.Figure8 shows the J-V characteristics of the DSCs before and after improvement by the intercalation of the Ag nanoparticles into the TiO2 electrodes. The optimum size of the Ag nanoparticle of 19.16 nm was found to give the maximum JSC and the maximum efficiency of the DSCs. The intercalation of the Ag nanoparticles to the TiO2 layer has been shown not to significantly affect values of VOC, Figure 7, because the VOC is determined by the redox potential and the Fermi energy of semiconductors [1, 36], which do not change significantly with the change in size of the Ag nanoparticles.Figure9 shows the short-term stability of the dye-sensitized solar cells which were kept in an ambient atmosphere. The J-V characteristics of dye-sensitized solar cell using the Ag nanoparticle size of 19.16 nm on the TiO2 electrode were measured at 24 h interval. It was found that the efficiency of the dye-sensitized solar cells was slightly enhanced in the first  3 days because of the increases in VOC and FF increase. However, from the  4th day, the efficiency of dyesensitized of solar cells began to decrease because of the decrease in short circuit current density. This could be due to the instability of the Ag nanoparticles in the I-/I3- redox electrolyte [1].Variation of (a) open-circuit voltage (VOC) and short-circuit current density (JSC), (b) fill factor (FF) and energy conversion efficiency of DSC with TiO2/Ag (19.16 nm) electrode during a short-term stability test.
(a)(b)


## 3.1. Morphology of the TiO2/Ag Deposited Films

The TiO2 films were prepared by screen printing 3 layers of the TiO2 paste and calcination at 450°C for 30 minutes. A thickness measured using SEM is approximately 13.8 μm as shown in Figure 1 (in agreement with [27–30]).The TiO2 films were loaded with the Ag nanoparticles using the AgNO3 soaking and the UV illumination treatment described in the experimental part 2.2. After the films were irradiated by the UV light, they turned brownish grey in a few minutes due to photocatalytic reduction of Ag+ to Ag [31]. The Ag nanoparticles on the TiO2 particles were not readily observed by the SEM (Figure 2). However, The TiO2/Ag composite films were characterized using energy dispersive X-Ray spectroscopy (EDX) technique attached to the SEM. We found that the peaks of the Ag nanoparticles were present (Figure 2), suggesting the presence of the Ag nanoparticles on surface of the TiO2 films.Figure 2
An SEM cross-sectional micrograph of the TiO2/Ag composite film with a UV exposure for 120 minutes. Inset shows an EDX spectrum indicating the presence of the Ag nanoparticles on the TiO2 films.Figure3(a) shows a TEM micrograph of the TiO2 nanoparticles from the TiO2 films before immersion in the AgNO3 solution. We found that the TiO2 nanoparticles were nanorods and the lengths were approximately 25 nm. Figure 3(b) shows an example of the TEM images of the TiO2 nanorods from the films after immersion in the AgNO3 solution and exposed to the UV irradiation for 120 minutes. The result shows the presence of the TiO2 nanorods and the spherical Ag nanoparticles adsorbed on surfaces of the TiO2 nanorods. An example of XRD pattern of the TiO2/Ag composite films (Figure 4) shows that four 2θ diffraction peaks at 38.12, 44.30, 64.44, and 77.40 could, respectively, be indexed as (111), (200), (220), and (311) planes of face-centered cubic Ag. Peaks at 25.36, 37.05, 37.90, 48.15, and 54.05 are indexed as (101), (103), (004), (200), and (105) planes of the anatase TiO2.TEM micrographs of the TiO2 nanotubes  (a) before and (b) after immersion in the AgNO3 solution with UV exposure for  120 minutes.
(a)(b)Figure 4
XRD peaks of the TiO2/Ag composite film with UV exposure for 120 minutes on an FTO glass substrate. (Note: graph plotted by OriginLab software program.)The Ag nanoparticles were also prepared on the carbon-coated copper grids and exposed to varied UV exposure times of 0, 5, 10, 15, 20, 30, 60, 90, 120, 150, 180 and 240 minutes. The average diameters of the Ag nanoparticles measured from the TEM micrographs using Image-Pro Plus 5.0 software program were approximately4.36±2.53, 4.56±1.78, 5.39±1.83, 6.20±1.65, 7.17±2.59, 10.98±1.80, 15.57±3.26, 19.16±3.71, 23.55±4.26, 27.51±8.05, and  38.56±5.30, respectively. The sizes of Ag nanoparticles were found to depend strongly on the UV exposure time (Figure 5) due to the photocatalytic reduction of the Ag+ to the Ag metal in the form of the Ag nanoparticles where electrons were provided by water [17, 31].TEM micrographs and size distributions of silver nanoparticles prepared by photocatalytic reduction in a 0.1 M AgNO3 solution on the carbon-coated copper grids at UV exposure times of (a) 5 minutes, (b) 120 minutes, and (c) 240 minutes, respectively. The average size increases and the distribution broadens with an increase in the UV exposure time. (Note: graph plotted by OriginLab software program).
(a)(b)(c)


## 3.2. The Effect of the Ag Nanoparticle Size on Optical Absorption Spectra

The absorption spectrum of the Ag nanoparticles exhibits the surface plasmon peak at approximately 400 nm on the broad band [32]. Optical absorption spectra can be theoretically calculated using Mie's theory. When the particles having diameter (R) are suspended in a medium with the dielectric constant (εm), the dipolar absorption efficiency (Qabs) is given by(1)Qabs=24πRλ⋅εm3/2ε′′(ω)ε′′(ω)2+〈ε′(ω)+2εm+48π2R2εm2/5λ2〉2,
where λ is a wavelength of the incoming light in the medium, and ε′(ω) and ε′′(ω) represent the real and imaginary parts of the dielectric function, ε(ω), respectively, [ε(ω)=ε′(ω)+ε′′(ω)].  Thus, the absorption efficiency of particles is a function of the dielectric constant of the metal, that of medium and the size of the particle.From (1), the Mie's theory only successfully explains the absorption band for metallic nanoparticles in visible range, and,for radius less than 5 nm, the width of the surface plasmon peak increases linearly with the reciprocal of the radius [32, 33]. On the other hand, the width of the surface plasmon peak increases with an increase in the radius in the range larger than 10 nm, because of inhomogeneous polarization of the particles in the electromagnetic field of the incoming light due to excitation of a different multiple modes which makes a peak in the spectrum at a different energy [32, 34]. Figure 6(a) shows optical absorption spectra of the Ag nanoparticles films indicating an increase in wavelength (red shifted) with an increase in the diameters of the Ag nanoparticles because the width of the surface plasmon peak increases.Optical absorption spectra of: (a) the Ag nanoparticle films with various particle sizes of the Ag nanoparticles in the range of 4.36–38.56 nm and (b) the Ag/N719 dye film compared with an optical absorption spectrum of3×10-5 M N719 dye solution.
(a)(b)Figure6(b) shows the absorption peak of the Ag/N719 dye film, it is found that the Ag 19.16 nm/N719dye film has a maximum peak width or red shift due to the surface plasmon resonance of the silver particles contributing to the absorption coefficient of the dye. The absorption of the Ru-dye can occur via the metal-ligand charge-transfer transition (MLCT), t2→π* MLCT transitions in the absorption maximum at 396 and 534 nm, and π→π* intraligand transition in the UV [35]. Thus, both the surface Plasmon resonance absorption of Ag nanoparticles and the Ru-dye absorption for MLCT transition contributed to the total absorption.


## 3.3. The Effect of the Ag Nanoparticle Size on Efficiency of the DSCs

Parameters extracted fromJ-V characteristics, for example, Figure 8, of the TiO2/Ag composite film electrode DSCs are shown in Table 1. The Ag nanoparticles of the average size of 19.16 nm (3.59±0.50 weight % of Ag nanoparticles in the TiO2/Ag composite) were found to result in the maximum value of short circuit current density of 8.12 mA/cm2.Table 1
Weight (%) of Ag nanoparticles obtained from SEM-EDX analysis, short circuit current densities (JSC), open circuit voltages (VOC), fill factors (FF), and efficiencies of DSCs prepared using the TiO2/Ag composite film electrodes compared with pure TiO2 electrode (reference) under AM1.5.
No.Size of Agnanoparticles on TiO2 electrode (nm)Weight (%) of Ag nanoparticlesJSC (mA/cm2)VOC (V)FFEfficiency (%)1pure TiO2 (reference)07.500.720.754.0224.36±2.533.30±0.357.070.750.764.0234.56±1.784.01±0.568.110.740.684.0745.39±1.833.52±0.277.210.760.623.4056.20±1.653.45±0.307.840.740.623.6467.17±2.593.56±0.306.810.780.633.34710.98±1.803.54±0.386.320.770.783.82812.5 [18]—4.400.810.692.5915.57±3.263.29±0.116.810.750.783.981019.16±3.713.59±0.508.120.730.804.761123.55±4.264.14±0.946.430.760.753.641227.51±8.054.20±0.346.040.760.763.511338.56±5.304.42±0.456.190.740.753.431440 [19]—11.530.650.534.1015~100 [20]—2.100.820.540.93As shown in Table1, the pure TiO2 electrode (reference cell) results in the short circuit current density (JSC) of 7.50 mA/cm2, open circuit voltages (VOC) of 0.72 V, fill factors (FF) of 0.75, and efficiency of 4.02%. For the TiO2/Ag electrodes, after improvement with intercalation of Ag nanoparticles of which size ranging from 4.36 to 38.56 nm, we found that the dye-sensitized solar cell which was prepared from the TiO2/Ag (19.16 nm) electrode had maximum values of the JSC, FF, and efficiency of 8.12 mA/cm2, 0.80 and 4.76%, respectively, with VOC of 0.73. Compared with the reference cell, the TiO2/Ag (19.16 nm) is found to improve JSC, FF, and efficiency because of an optimum electromagnetic field introduced by the silver plasmon resonance that enhances the optical absorption of the dye [2, 3, 36]. The other possible reason is that the Ag nanoparticles have a catalytic effect that increases the reaction rate between the semiconductor, dye, and the redox electrolyte and/or the internal photoemission from the Ag nanoparticles increases the photocurrent [1, 3, 36]. However, the dye-sensitized solar cells which were prepared from the TiO2/Ag electrodes with the Ag nanoparticle sizes bigger than 19.16 nm have low values of the JSC. It is believed that with the Ag particle sizes bigger than 19.16 nm, Schottky barriers formed at the TiO2/Ag contacts become dominant and retard electron transport in the conduction bands [1, 3, 37, 38].Figure7 plots JSC, VOC, FF, and efficiencies versus the sizes of the Ag nanoparticles. The DSCs in our study were compared with the Ag nanoparticle size of around 12.5 [18], 40 [19], and 100 [20] nm on the TiO2 electrodes reported elsewhere. Due to different thicknesses of the TiO2 layers prepared, direct comparison cannot be made. However, the improved JSC of the best DSC prepared in this study is noteworthy. Compared with the reported DSCs with the Ag nanowires of 40 nm in diameter and 20 μm in length [19] with the JSC of 11.53 mA/cm2, the best DSC in this study has a lower value of JSC. The high value of JSC in the Ag nanowire DSCs has been reported to be due to metal network formation by adding Ag nanowires to improve the production and transportation of photon-generated current [39].Figure 7
Open circuit voltages (VOC), short circuit current densities (JSC), fill factors (FF), and efficiencies of the DSCs  with varied sizes of the Ag nanoparticles compared with reported  DSCs [18–20]. At [18], use 2 μm of TiO2 thickness and size of 0.25 cm2, [19] use 15 μm of TiO2 thickness and size of 0.25 cm2, [20] use 8.1 μm of TiO2 thickness and size of 4.0 cm2, and this study uses 13.8 μm of TiO2 thickness and size of 0.6 cm2.Figure 8
J-V characteristics of the DSCs composed of the TiO2 electrodes with N719 dye before and after improvement with the Ag nanoparticles.However theVOC, FF, and efficiency values of the Ag nanowire DSCs are not higher than the best value reported in this study. When compared with the reported DSCs with the Ag nanoparticle size of around 100 nm [20], the values of JSC, VOC, FF and Efficiency follow a decreasing trend after the maximum values because the Schottky barriers formed at the TiO2/Ag contact retarding electron transport in conduction bands [1, 3]. Therefore, the Ag nanoparticles size of 19.16 nm prepared in this study is an appropriate size to improve JSC of the DSCs.Figure8 shows the J-V characteristics of the DSCs before and after improvement by the intercalation of the Ag nanoparticles into the TiO2 electrodes. The optimum size of the Ag nanoparticle of 19.16 nm was found to give the maximum JSC and the maximum efficiency of the DSCs. The intercalation of the Ag nanoparticles to the TiO2 layer has been shown not to significantly affect values of VOC, Figure 7, because the VOC is determined by the redox potential and the Fermi energy of semiconductors [1, 36], which do not change significantly with the change in size of the Ag nanoparticles.Figure9 shows the short-term stability of the dye-sensitized solar cells which were kept in an ambient atmosphere. The J-V characteristics of dye-sensitized solar cell using the Ag nanoparticle size of 19.16 nm on the TiO2 electrode were measured at 24 h interval. It was found that the efficiency of the dye-sensitized solar cells was slightly enhanced in the first  3 days because of the increases in VOC and FF increase. However, from the  4th day, the efficiency of dyesensitized of solar cells began to decrease because of the decrease in short circuit current density. This could be due to the instability of the Ag nanoparticles in the I-/I3- redox electrolyte [1].Variation of (a) open-circuit voltage (VOC) and short-circuit current density (JSC), (b) fill factor (FF) and energy conversion efficiency of DSC with TiO2/Ag (19.16 nm) electrode during a short-term stability test.
(a)(b)


## 4. Conclusion

The DSCs composed of mesoporous TiO2 films, N719 Ru dye and the redox of I−/I3- were prepared and improved by the intercalation of the Ag nanoparticles into the TiO2 electrodes by photoreduction method. The Ag nanoparticles were face centered cubic and varied in size in the range of 4.36–38.65 nm. The TiO2/Ag composite films were characterized by XRD, SEM, TEM and UV-Vis Spectrophotometer. The optimum size of the Ag nanoparticles was 19.16 nm giving the maximum JSC and efficiency of 8.12 mA/cm2 and 4.76%, respectively.



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*Source: 258635-2011-06-28.xml*