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<art><ui>1556-276X-7-147</ui><ji>1556-276X</ji><fm>
<dochead>Nano Express</dochead>
<bibl>
<title>
<p>Preparation, characterization, and application of titanium nano-tube array in dye-sensitized solar cells</p>
</title>
<aug>
<au id="A1"><snm>Ho</snm><fnm>Shih-Yu</fnm><insr iid="I1"/><email>stacy760414@hotmail.com</email></au>
<au id="A2" ca="yes"><snm>Su</snm><fnm>Chaochin</fnm><insr iid="I1"/><email>f10913@ntut.edu.tw</email></au>
<au id="A3"><snm>Cheng</snm><fnm>Chieh-Chung</fnm><insr iid="I1"/><email>kalston2003@hotmail.com</email></au>
<au id="A4"><snm>Kathirvel</snm><fnm>Sasipriya</fnm><insr iid="I1"/><email>ksasipriya@gmail.com</email></au>
<au id="A5"><snm>Li</snm><fnm>Chung-Yen</fnm><insr iid="I2"/><email>952203004@cc.ncu.edu.tw</email></au>
<au id="A6" ca="yes"><snm>Li</snm><fnm>Wen-Ren</fnm><insr iid="I2"/><email>ch01@ncu.edu.tw</email></au>
</aug>
<insg>
<ins id="I1"><p>Institute of Organic and Polymeric Materials, National Taipei University of Technology, Taipei, 10608, Taiwan, Republic of China</p></ins>
<ins id="I2"><p>Department of Chemistry, National Central University, Chung-Li, 32001, Taiwan, Republic of China</p></ins>
</insg>
<source>Nanoscale Research Letters</source>
<issn>1556-276X</issn>
<pubdate>2012</pubdate>
<volume>7</volume>
<issue>1</issue>
<fpage>147</fpage>
<url>http://www.nanoscalereslett.com/content/7/1/147</url>
<xrefbib><pubidlist><pubid idtype="doi">10.1186/1556-276X-7-147</pubid><pubid idtype="pmpid">22353282</pubid></pubidlist></xrefbib>
</bibl>
<history><rec><date><day>30</day><month>11</month><year>2011</year></date></rec><acc><date><day>21</day><month>2</month><year>2012</year></date></acc><pub><date><day>21</day><month>2</month><year>2012</year></date></pub></history>
<cpyrt><year>2012</year><collab>Ho et al; licensee Springer.</collab><note>This is an Open Access article distributed under the terms of the Creative Commons Attribution License (<url>http://creativecommons.org/licenses/by/2.0</url>), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.</note></cpyrt>
<kwdg>
<kwd>TiO<sub>2</sub>
</kwd>
<kwd>titanium tetrachloride</kwd>
<kwd>titanium (IV) <it>n</it>-butoxide</kwd>
<kwd>nano-tube</kwd>
<kwd>anodization</kwd>
<kwd>DSSCs</kwd>
</kwdg>
<abs>
<sec>
<st>
<p>Abstract</p>
</st>
<p>The vertically orientated TiO<sub>2 </sub>nanotube array (TNA) decorated with TiO<sub>2 </sub>nano-particles was successfully fabricated by electrochemically anodizing titanium (Ti) foils followed by Ti-precursor post-treatment and annealing process. The TNA morphology characterized by SEM and TEM was found to be filled with TiO<sub>2 </sub>nano-particles interior and exterior of the TiO<sub>2 </sub>nano-tubes after titanium (IV) <it>n</it>-butoxide (TnB) treatment, whereas TiO<sub>2 </sub>nano-particles were only found inside of TiO<sub>2 </sub>nano-tubes upon titanium tetrachloride (TiCl<sub>4</sub>) treatment. The efficiency in TNA-based DSSCs was improved by both TnB and TiCl<sub>4 </sub>treatment presumably due to the increase of dye adsorption.</p>
</sec>
</abs>
</fm><bdy>
<sec>
<st>
<p>Introduction</p>
</st>
<p>Since O'Regan and Gr&#228;tzel reported highly efficient TiO<sub>2</sub>-based dye-sensitized solar cells (DSSCs) in 1991, many attempts have been made to sensitize titanium dioxide (TiO<sub>2</sub>) nano-scale films. TiO<sub>2 </sub>nano-particulate films are typically preferred as they provide a high surface area for dye adsorption, leading to high photocurrent conversion efficiency. Due to the three-dimensional transport path, TiO<sub>2 </sub>nano-particulate films brought higher electron recombination and met larger grain boundary among interconnected nano-particles. In this research, we have fabricated vertically orientated one-dimensional nano-structure TiO<sub>2 </sub>nano-tube array (TNA) by electrochemical anodization. The TNA-based DSSCs were expected to have a better performance than the nano-particulate-based DSSCs due to the better electron transportation and recombination property. However, due to the less surface area of TiO<sub>2 </sub>nano-tube array, the efficiency of TNA-based DSSCs is still lower than that of TiO<sub>2 </sub>nano-particle-based DSSCs. Post-treatment of TNA by Ti precursors to form a TiO<sub>2 </sub>nano-particulate layers on TNA became a strategy which could increase the TiO<sub>2 </sub>surface area for more dye adsorption. This research showed that the DSSCs fabricated by TNA after post-treatment by titanium tetrachloride (TiCl<sub>4</sub>) and TiO<sub>2 </sub>nano-tubes after titanium (IV) <it>n</it>-butoxide (TnB) raised up the photocurrent conversion efficiency.</p>
<p>DSSCs have aroused intense interest over the past few years because they have been demonstrated to be able to achieve high solar-to-electric energy conversion efficiency with low-cost manufacture process and materials. In DSSCs, the photoelectrodes are made of porous semiconductor layers chemisorbed with an organic sensitizer. When DSSCs are illuminated with sun light, the photoelectron of the sensitizer is ejected into the semiconductor films and sent to the external circuit. The redox pairs in the electrolyte transport the holes from the oxidized dye molecules to the counter electrode to complete the electric cycle <abbrgrp>
<abbr bid="B1">1</abbr>
</abbrgrp>. TiO<sub>2 </sub>is one of the most promising semiconductor materials in preparing the photoanodes for DSSCs due to its wide band gap characteristics and unique photoelectric properties <abbrgrp>
<abbr bid="B2">2</abbr>
</abbrgrp>. TiO<sub>2 </sub>nano-particulate films are preferred as they provide a high surface area for dye adsorption, leading to high photocurrent conversion efficiency. The electron-collecting TiO<sub>2 </sub>layer in DSSCs is typically 10 to 15 &#956;m thick with a three-dimensional network of interconnected nano-particles. However, TiO<sub>2 </sub>nano-crystalline films acquire long electron transport path and larger grain boundary between nano-particles <abbrgrp>
<abbr bid="B3">3</abbr>
<abbr bid="B4">4</abbr>
</abbrgrp>. This would hinder the electron collection efficiency and limit the performance of DSSCs. It was proposed that one-dimensional TNA aligned perpendicular to photoanode substrate could enhance the electron transportation and, thus, lower the possibility of electron recombination with redox electrolytes, leading to the higher photo-to-electron conversion efficiency <abbrgrp>
<abbr bid="B3">3</abbr>
<abbr bid="B4">4</abbr>
<abbr bid="B5">5</abbr>
</abbrgrp>. The TNA has been first prepared by Zwilling et al. using the electrochemical anodization method <abbrgrp>
<abbr bid="B6">6</abbr>
</abbrgrp>. The TNA morphology, including tube length, hole diameter, and wall thickness, can be systematically controlled by varying the anodization parameters, such as anodization potential, electrolyte, and pH value <abbrgrp>
<abbr bid="B7">7</abbr>
<abbr bid="B8">8</abbr>
</abbrgrp>. Zhu et al. had investigated the dynamics of electron transport and recombination properties of the oriented TiO<sub>2 </sub>nano-tube structure in DSSCs by frequency-resolved modulated photocurrent/photovoltage spectroscopies and found the higher charge-collection efficiency and slower electron recombination in the TiO<sub>2 </sub>nano-tube-based DSSCs than the TiO<sub>2 </sub>nano-particle-based counterparts <abbrgrp>
<abbr bid="B3">3</abbr>
</abbrgrp>. One of the reasons for improving the performance of the DSSCs is considered to be due to the increase of the amount of the dye adsorbed onto the TiO<sub>2 </sub>surface of photoelectrodes in DSSCs. In order to increase the surface area of TiO<sub>2 </sub>electrodes, post-treatment of TNA to form an extra layer of TiO<sub>2 </sub>nano-particles has been applied <abbrgrp>
<abbr bid="B9">9</abbr>
<abbr bid="B10">10</abbr>
<abbr bid="B11">11</abbr>
</abbrgrp>. In this work, we compared the effect of post-treatment of anodic TNA by different Ti-precursors on the TNA morphology and the resulting DSSCs performance.</p>
</sec>
<sec>
<st>
<p>Experimental details</p>
</st>
<sec>
<st>
<p>Preparation, modification, and characterization of anodic TNA</p>
</st>
<p>Titanium foils with thickness of 0.25 mm (99.5% purity; Alfa Aesar, Ward Hill, MA, USA) were used for anodic growth of TNA. Titanium foils were first polished by sonication in chemical polishing solvent which contained nitric acid, ammonia fluoride, urea, ethanol, and hydrogen peroxide in 12:5:5:3:12 <it>v/v </it>ratio and rinsed subsequently with deionized (DI) water, acetone, and methanol. The anodization reaction was carried out in a two-electrode electrochemical cell with polished Ti foil (2 &#215; 2.5 cm<sup>2</sup>) which served as the anode-working electrode and Pt foil (thickness 0.025 mm; Alfa Aesar) as the counter electrode. The separation between Ti electrode and Pt electrode was about 3.5 cm. The anodization electrolyte contains 0.3 wt% NH<sub>4</sub>F and 2 vol% H<sub>2</sub>O in ethylene glycol solution. The anodization was operated under a constant potential of 60 V at low temperature of 15&#176;C with magnetic stirring. The reaction period controlled the thickness of TiO<sub>2 </sub>nano-tube arrays. Typically the TNA samples with tube length of approximately 15 &#956;m were obtained after 2 h of anodization process. It is evident that increasing the TNA length leads to the increase of short-circuit photocurrent density due to the higher surface area available for dye adsorption. The TNA foils were then carefully washed with deionized water to remove the surface residual electrolyte in the nano-tube arrays. Such prepared TNA samples were then annealed at 450&#176;C for 3 h with a heating rate of 1&#176;C/min in order to transform the TNA from amorphous to anatase crystalline phase.</p>
<p>Figure <figr fid="F1">1</figr> summarizes the procedures for post-treatment of annealed TNA. The TiCl<sub>4</sub>-treated TNA (TNA-TiCl<sub>4</sub>) was prepared from annealed TNA which was soaked in 0.2 M TiCl<sub>4 </sub>solution (in ethanol) at 60&#176;C for 30 min followed by heat treatment at 450&#176;C for 30 min. The TnB-treated TNA (TNA-TnB) was prepared as follows: titanium (IV) <it>n</it>-butoxide (Ti(O-Bu)<sub>4</sub>, TnB) (ACROS Organics, New Jersey, USA) was mixed with 2 M CH<sub>3</sub>COOH (pH = 2.5) at room temperature under magnetic stirring for approximately 5 days until a homogeneous sol solution was obtained. The TiO<sub>2 </sub>sol and the annealed TNA were both transferred to a teflon-lined autoclave to perform the hydrothermal treatment at 200&#176;C for 5 h. The Ti foil was then removed from the autoclave, rinsed with DI water, and heated at 450&#176;C for 30 min to form TNA-TnB.</p>
<fig id="F1"><title><p>Figure 1</p></title><caption><p>Procedures for post-treatment of annealed TNA</p></caption><text>
   <p><b>Procedures for post-treatment of annealed TNA</b>. Fabrication flow chart of TNA-TiCl<sub>4 </sub>and TNA-TnB. TNA, TiO<sub>2 </sub>nano-tube array; DI-water, deionized water; XRD, X-ray diffraction; SEM, scanning electron microscopy.</p>
</text><graphic file="1556-276X-7-147-1"/></fig>
<p>The surface morphology and crystal phase of TNA, TNA-TiCl<sub>4</sub>, and TNA-TnB were investigated by scanning electron microscopy (SEM) (SM6500F, JEOL Ltd., Akishima, Tokyo, Japan) and X-ray diffraction (XRD) (PANalytical X'Pert PRO, Almelo, The Netherlands), respectively. The results were confirmed by high-resolution transmission electron microscopy (Hitachi H-7100, Hitachi Ltd., Chiyoda, Tokyo, Japan).</p>
</sec>
<sec>
<st>
<p>Dye-sensitized solar cell assemble and performance measurement</p>
</st>
<p>To fabricate DSSCs devices, three kinds of TNAs including TNA, TNA-TiCl<sub>4</sub>, and TNA-TnB, served as photoanodes, were combined with a transparent Pt counter electrode (cathode). The TNAs samples were sensitized by dye molecules (3 &#215; 10<sup>-4 </sup>M, N719 in a mixed solvent of acetonitrile and tertbutyl acohol (volume ratio = 1:1)) for 24 h. The amount of dye adsorbed on TNA electrodes was determined by desorbing the N719 from TNAs surfaces into a solution of 0.1 M NaOH. The concentration of the adsorbed N719 was analyzed by UV-visible spectrophotometer (V-630, JASCO Corp., Easton, MD, USA). The Pt cathode was made by a 'two-step dip coating' process developed by Wei et al. <abbrgrp>
<abbr bid="B12">12</abbr>
</abbrgrp>. We have first prepared the poly-<it>N</it>-vinyl-2-pyrrolidone (PVP)-capped Pt nano-particles by dissolving PVP (M.W. = 8000) and H<sub>2</sub>PtCl<sub>6 </sub>(Pt precursor) into deionized water at room temperature and well stirred until a light-yellow solution was obtained. A NaBH<sub>4 </sub>solution was then added drop by drop to the H<sub>2</sub>PtCl<sub>6</sub>-PVP solution, and the solution quickly turned into a black color, indicating the formation of Pt nano-particles (Pt-PVP solution).</p>
<p>FTO glass (8&#937;/sq., Solaronix SA, Aubonne VD, Switzerland) was pretreated by 1% ML-371 aqueous solution at room temperature for 1 min in order to increase adhesion between the PVP-capped Pt nano-particles and FTO surface. The ML-371-modified FTO substrate was then dipped into the Pt-PVP solution for 5 min and rinsed with deionized water followed by heat-treatment at 400&#176;C for 5 h to remove completely the organic component and complete the preparation of counter electrode.</p>
<p>To assemble the DSSCs, the liquid electrolyte of 0.1 M lithium iodide, 0.05 M iodine (I<sub>2</sub>), 0.5 M 4-tert-butylpyridine, 0.5 M 1,2-Dimethyl-3-propylimidazolium iodide in acetonitrile was applied to the above-prepared Pt electrode which was then placed over the N719-coated TNAs electrodes. The edges of the cells sealed with a hot-melt film (Surlyn, 125 &#956;m) and the electrolyte (I<sup>-</sup>/I<sub>2</sub>/I<sub>3</sub>
<sup>- </sup>redox couple) were injected into the space. The active cell area studied in this work is 0.25 cm<sup>2 </sup>(0.5 cm &#215; 0.5 cm). The photoelectrochemical performance of the resultant solar cells were measured by back illuminated through the Pt counter electrode due to the nonpenetration of light through the photoanode Ti metal substrate.</p>
<p>The current (I)-voltage (V) characteristics were performed using a digital source meter (Keithley model 2400, Keithley Instruments Inc., Cleveland, OH, USA) with the TNA-based DSSCs devices under one-sun AM 1.5 irradiation from a solar simulator (300 W Xe light and filters, Oriel Instruments, Irvine, CA, USA) on a 0.25 cm<sup>2 </sup>sample area.</p>
</sec>
</sec>
<sec>
<st>
<p>Results and discussion</p>
</st>
<sec>
<st>
<p>Formation and characterization of anodic titanium oxide nano-tube arrays</p>
</st>
<p>TiO<sub>2 </sub>electrode is one of the major concerns in DSSCs application. Since the TiO<sub>2 </sub>phase, morphology, and surface area of TiO<sub>2 </sub>films will affect the dye adsorption, electron transport, and electrolyte diffusion in the cell as well as the DSSCs performance. In this work, we have devised two kinds of Ti-precursor solutions to fabricate TiO<sub>2 </sub>nano-particles decorated TNA on Ti substrates which can serve as photoanodes for DSSCs device. During the optimization stage of anodization process, the important roles of the anodization condition, including the thickness of Ti-foil (0.05-0.25 mm), temperature (15-30&#176;C), anodization potential (20-60 V), reaction period (10 min-24 h), and various kinds of F-containing electrolytes (HF, KF, and NH<sub>4</sub>F) in controlling the thickness (length of TiO<sub>2 </sub>nano-tubes), homogeneity, and morphology of TNA were revealed. The data presented below were obtained with NH<sub>4</sub>F/H<sub>2</sub>O/ethylene glycol electrolyte solution after anodization procedure at 15&#176;C for 2 h. Figure <figr fid="F2">2</figr> shows a typical current-time plot recorded during the constant potential anodization process. Within the first few seconds, the current dropped drastically to a local minimum indicating the oxidation of Ti-foil to form surface pits acting as nucleation sites for tube formation <abbrgrp>
<abbr bid="B13">13</abbr>
</abbrgrp>. Upon increasing the pit density, the current increased to a maximum where the pit density reached saturation. After further anodization, the current gradually decreased due to the continuously lengthen of TiO<sub>2 </sub>nano-tubes. Such anodization behavior is commonly observed in the self-organized pore formation process <abbrgrp>
<abbr bid="B14">14</abbr>
</abbrgrp> in which the competition between TiO<sub>2 </sub>oxide layer formation and dissolution of titanium progressed concurrently. Finally, the formation of vertically oriented TNA was achieved. The initially grown TNA was gray, which turned to yellow color after annealing at 450&#176;C for 3 h.</p>
<fig id="F2"><title><p>Figure 2</p></title><caption><p>Current-time plot of the constant potential anodization process</p></caption><text>
   <p><b>Current-time plot of the constant potential anodization process</b>. Current-time plot recorded during the constant potential anodization process.</p>
</text><graphic file="1556-276X-7-147-2"/></fig>
<p>Figure <figr fid="F3">3a</figr> shows the SEM images of the untreated TNA formed by anodizing a titanium foil with two types of magnification: 10,000&#215; (top view) and 50,000&#215; (side view, inset). The SEM image of lower magnification of TNA (Figure <figr fid="F3">3a</figr>) shows high porosity character of anodic TiO<sub>2 </sub>films with some nano-scale cracks. The higher magnification image of TNA (inset of Figure <figr fid="F3">3a</figr>) shows the self-organized TiO<sub>2 </sub>nano-tubes aligned densely with hexagonal close-packed arrangement. The inner diameters of these TiO<sub>2 </sub>nano-tubes based on SEM images are in the range of 100-120 nm, and the wall thickness is approximately 10 nm. The thickness of TNA corresponding to the length of TiO<sub>2 </sub>nano-tubes is about 15 &#956;m obtained from the SEM cross section analysis shown in Figure <figr fid="F4">4</figr>. It is consistent with other research works that high-aspect-ratio TiO<sub>2 </sub>nano-tubes can be fabricated with rapid growth rate by anodization <abbrgrp>
<abbr bid="B4">4</abbr>
<abbr bid="B9">9</abbr>
<abbr bid="B15">15</abbr>
</abbrgrp>.</p>
<fig id="F3"><title><p>Figure 3</p></title><caption><p>SEM images of top view of (a) TNA, (b) TNA-TiCl<sub>4</sub>, and (c) TNA-TnB</p></caption><text>
   <p><b>SEM images of top view of (a) TNA, (b) TNA-TiCl<sub>4</sub>, and (c) TNA-TnB</b>. The inset images are the side view of (a) TNA, (b) TNA-TiCl<sub>4</sub>, and (c) TNA-TnB. TNA, TiO<sub>2 </sub>nano-tube array; TNA-TnB, TiO<sub>2 </sub>nano-tubes after titanium (IV) <it>n</it>-butoxide treatment; TNA-TiCl<sub>4</sub>, TiO<sub>2 </sub>nano-tubes after titanium tetrachloride treatment.</p>
</text><graphic file="1556-276X-7-147-3"/></fig>
<fig id="F4"><title><p>Figure 4</p></title><caption><p>SEM cross sectional view of annealed-TNA</p></caption><text>
   <p><b>SEM cross sectional view of annealed-TNA</b>. Mag, magnification; WD, width; EHT, extra high tension.</p>
</text><graphic file="1556-276X-7-147-4"/></fig>
<p>Figure <figr fid="F3">3b, c</figr> shows the top-view SEM images of the decorated TNAs after post-treatment by TiCl<sub>4 </sub>and TnB solution, respectively, with the corresponding side view images with higher magnification as shown in the inset of Figure <figr fid="F3">3b, c</figr>. The length of TiO<sub>2 </sub>nano-tubes remains the same after different post-treatment. For both TiCl<sub>4 </sub>and TnB treated TNAs samples (denoted as TNA-TiCl<sub>4 </sub>and TNA-TnB), additional materials can be observed on the top of TNAs and inside the TiO<sub>2 </sub>nano-tubes. Yet, outside the TnB-treated TNA, the TiO<sub>2 </sub>nano-tubes were apparently coated with an extra layer of TiO<sub>2 </sub>nano-particles. Transmission electron microscope (TEM) experiments had been performed on TNA-TiCl<sub>4 </sub>and TNA-TnB samples detached from the Ti foil and dispersed on a copper grid. The bulk crystallites were observed (Figure <figr fid="F5">5a</figr>) inside TiO<sub>2 </sub>nano-tubes in the case of TiCl<sub>4</sub>-treated TNA sample. In TnB-treated TNA, bulk crystallites were observed both inside and outside the nano-tubes as shown in Figure <figr fid="F5">5b</figr>. The average inner diameter of TiO<sub>2 </sub>nano-tubes in TNA-TiCl<sub>4 </sub>and TNA-TnB after different post-treatment was about 85-120 nm based on TEM analysis which is consistent with SEM results.</p>
<fig id="F5"><title><p>Figure 5</p></title><caption><p>TEM images of (a) TNA-TiCl<sub>4 </sub>and (b) TNA-TnB</p></caption><text>
   <p><b>TEM images of (a) TNA-TiCl<sub>4 </sub>and (b) TNA-TnB</b>. TEM, transmission electron microscope; TNA, TiO<sub>2 </sub>nano-tube array; TNA-TnB, TiO<sub>2 </sub>nano-tubes after titanium (IV) <it>n</it>-butoxide treatment; TNA-TiCl<sub>4</sub>, TiO<sub>2 </sub>nano-tubes after titanium tetrachloride treatment.</p>
</text><graphic file="1556-276X-7-147-5"/></fig>
<p>XRD was used to confirm the crystalline phase of TiO<sub>2 </sub>nano-structure. Figure <figr fid="F6">6</figr> shows the XRD patterns of (a) as-prepared TNA, (b) annealed-TNA, (c) TiCl<sub>4</sub>-treated TNA, and (d) TnB-treated TNA. The as-prepared TNA (before annealing) were amorphous (Figure <figr fid="F6">6a</figr>). Upon annealing to 450&#176;C, the sharp anatase diffraction peaks appeared (Figure <figr fid="F6">6b</figr>) with crystal domain of approximately 20 nm. After post-treatment by TiCl<sub>4 </sub>and TnB, the XRD patterns remain the same for both TNA-TiCl<sub>4 </sub>and TNA-TnB, suggesting that the TiO<sub>2 </sub>crystalline phase was not affected by post-treatment. The slight increase of TiO<sub>2 </sub>crystal domain to 22 nm (for TNA-TiCl<sub>4</sub>) and 29 nm (for TNA-TnB) was due to the two times annealing at 450&#176;C for post-treated TNAs samples.</p>
<fig id="F6"><title><p>Figure 6</p></title><caption><p>XRD patterns of (a) as-prepared TNA, (b) annealed-TNA, (c) TiCl<sub>4</sub>-treated TNA, and (d) TnB-treated TNA</p></caption><text>
   <p><b>XRD patterns of (a) as-prepared TNA, (b) annealed-TNA, (c) TiCl<sub>4</sub>-treated TNA, and (d) TnB-treated TNA</b>. XRD, X-ray diffraction; TNA, TiO<sub>2 </sub>nano-tube array; TNA-TnB, TiO<sub>2 </sub>nano-tubes after titanium (IV) <it>n</it>-butoxide treatment; TNA-TiCl<sub>4</sub>, TiO<sub>2 </sub>nano-tubes after titanium tetrachloride treatment; A, anatase diffraction peak.</p>
</text><graphic file="1556-276X-7-147-6"/></fig>
</sec>
<sec>
<st>
<p>Application of anodic TNA electrodes to DSSCs and photoelectrochemical performance study</p>
</st>
<p>The above-prepared TiO<sub>2 </sub>nano-tube arrays (TNA, TNA-TiCl<sub>4</sub>, and TNA-TnB) were used to fabricate the DSSCs for photoelectrochemical performance study. The results obtained from I-V curve measurements for N719-sensitized DSSCs under simulated AM 1.5 illumination is shown in Figure <figr fid="F7">7</figr>. The thickness of TNAs layers on Ti foil was fixed at approximately 15 &#956;m. Table <tblr tid="T1">1</tblr> lists the TNAs thickness, the amount of dye adsorbed on TNAs layers (N719<sub>ads</sub>), and photoelectric data of the DSSCs in Figure <figr fid="F7">7</figr> including the open circuit voltage, the short-circuit photocurrent density (J<sub>sc</sub>), the fill factor, and the photocurrent conversion efficiency (<it>&#951;</it>). It is apparent that by post-treatment of the TNA, the performance of DSSCs was notably enhanced. The device based on the untreated TNA has shown the lowest J<sub>sc </sub>(3.84 mA/cm<sup>2</sup>) and <it>&#951; </it>(1.38%). This is due to the low surface area of the untreated TNA which uptakes less amount of dye molecules (0.092 &#956;mole/cm<sup>2</sup>). Higher efficiency and current density of DSSCs device might be attributed to the higher amount of adsorbed N719 and the fast electron transportation on TiO<sub>2 </sub>electrodes. As shown in Table <tblr tid="T1">1</tblr>, TnB treatment assisted the higher dye adsorption amount, raised from 0.092 to 0.116 &#956;mole/cm<sup>2 </sup>(approximately 26% increase of N719<sub>ads</sub>), and J<sub>sc </sub>also raised from 3.84 to 5.97 mA/cm<sup>2 </sup>(approximately 55% increase of J<sub>sc</sub>). Both results lead to the efficiency improvement from 1.38% to 2.40% (approximately 74% increase of <it>&#951;</it>). The significant increase of dye adsorption is due to the increased surface area from the decorated TiO<sub>2 </sub>nano-particles on TNA, as clearly seen from the SEM images (Figure <figr fid="F3">3c</figr>). TEM images (Figure <figr fid="F5">5b</figr>) also vindicated the presence of bulk TiO<sub>2 </sub>crystallites inside and outside the TNA. The further increase of J<sub>sc </sub>as well as <it>&#951; </it>is attributed to the increase of TiO<sub>2 </sub>crystallinity of TNA-TnB, as evidenced by XRD. The dye loading for TNA-TiCl<sub>4 </sub>sample is lower compared to that of TNA-TnB because the TiO<sub>2 </sub>nano-particles only subsist inside the nano-tubes. The slightly higher efficiency of TNA-TiCl<sub>4</sub>-based DSSCs compared to the untreated TNA one is due to the better TiO<sub>2 </sub>crystallinity after two times annealing process. Variation in the performance of different devices might be due to the variations in the TiO<sub>2 </sub>tube length. Nevertheless, same trends were observed within each batch of device study.</p>
<fig id="F7"><title><p>Figure 7</p></title><caption><p>Photocurrent-voltage characteristics of DSSCs made by TNA, TNA-TiCl<sub>4</sub>, and TNA-TnB</p></caption><text>
   <p><b>Photocurrent-voltage characteristics of DSSCs made by TNA, TNA-TiCl<sub>4</sub>, and TNA-TnB</b>. TNA, TiO<sub>2 </sub>nano-tube array; TNA-TnB, TiO<sub>2 </sub>nano-tubes after titanium (IV) <it>n</it>-butoxide treatment; TNA-TiCl<sub>4</sub>, TiO<sub>2 </sub>nano-tubes after titanium tetrachloride treatment.</p>
</text><graphic file="1556-276X-7-147-7"/></fig>
<tbl id="T1"><title><p>Table 1</p></title><caption><p>The I-V characterization of TNAs-based DSSCs</p></caption><tblbdy cols="7">
      <r>
         <c ca="left">
            <p>
               <b>Sample</b>
            </p>
         </c>
         <c ca="left">
            <p>
               <b>N719ads</b>
            </p>
            <p>
               <b>&#956;mole/cm<sup>2</sup></b>
            </p>
         </c>
         <c ca="left">
            <p>
               <b>Film thickness</b>
            </p>
            <p>
               <b>(&#951;m)</b>
            </p>
         </c>
         <c ca="left">
            <p>
               <b>Voc</b>
            </p>
            <p>
               <b>(V)</b>
            </p>
         </c>
         <c ca="left">
            <p>
               <b>Jsc</b>
            </p>
            <p>
               <b>(mA/cm<sup>2</sup>)</b>
            </p>
         </c>
         <c ca="left">
            <p>
               <b>FF</b>
            </p>
         </c>
         <c ca="left">
            <p/>
            <p>
               <b>&#951;</b>
            </p>
            <p>
               <b>(%)</b>
            </p>
         </c>
      </r>
      <r>
         <c cspan="7">
            <hr/>
         </c>
      </r>
      <r>
         <c ca="left">
            <p>TNA</p>
         </c>
         <c ca="left">
            <p>0.092</p>
         </c>
         <c ca="left">
            <p>14</p>
         </c>
         <c ca="left">
            <p>0.68</p>
         </c>
         <c ca="left">
            <p>3.84</p>
         </c>
         <c ca="left">
            <p>0.53</p>
         </c>
         <c ca="left">
            <p>1.38</p>
         </c>
      </r>
      <r>
         <c cspan="7">
            <hr/>
         </c>
      </r>
      <r>
         <c ca="left">
            <p>TNA-TiCl4</p>
         </c>
         <c ca="left">
            <p>0.096</p>
         </c>
         <c ca="left">
            <p>15</p>
         </c>
         <c ca="left">
            <p>0.66</p>
         </c>
         <c ca="left">
            <p>4.83</p>
         </c>
         <c ca="left">
            <p>0.51</p>
         </c>
         <c ca="left">
            <p>1.61</p>
         </c>
      </r>
      <r>
         <c cspan="7">
            <hr/>
         </c>
      </r>
      <r>
         <c ca="left">
            <p>TNA-TnB</p>
         </c>
         <c ca="left">
            <p>0.116</p>
         </c>
         <c ca="left">
            <p>16</p>
         </c>
         <c ca="left">
            <p>0.66</p>
         </c>
         <c ca="left">
            <p>5.97</p>
         </c>
         <c ca="left">
            <p>0.61</p>
         </c>
         <c ca="left">
            <p>2.40</p>
         </c>
      </r>
   </tblbdy></tbl>
</sec>
</sec>
<sec>
<st>
<p>Conclusions</p>
</st>
<p>The decorated TNAs were successfully fabricated by anodization method followed by titanium precursor post treatment. The morphology of TNA without post-treatment was observed from SEM and TEM images, typically approximately 15 &#956;m length, approximately 100 nm diameter, and 10 nm wall thickness were achieved after 2 h reaction. TNA with titanium precursor treatment alters the morphology which was confirmed from the SEM and TEM images. In the case of TNA-TnB, TiO<sub>2 </sub>nano-particles were filled interior and exterior of the TiO<sub>2 </sub>nano-tubes, whereas TiO<sub>2 </sub>nano-particles were filled only inside the TiO<sub>2 </sub>nano-tubes in TNA-TiCl<sub>4 </sub>upon TiCl<sub>4 </sub>treatment. An XRD pattern clearly indicates that the TNA, TNA-TiCl<sub>4</sub>, and TNA-TnB were pure anatase phase after annealing process at 450&#176;C. The photocurrent conversion efficiency of TNA-based, TNA-TiCl<sub>4</sub>-based, and TNA-TnB-based DSSCs was 1.38%, 1.61%, and 2.40%, respectively. The results showed that the DSSC efficiency in TNAs was enhanced by TiCl<sub>4 </sub>and TnB precursor post-treatment, presumably due to the increase of dye adsorption. The higher solar efficiency in TnB-doped DSSCs is due to the formation of extra layer of TiO<sub>2 </sub>nano-particles on TNA, leading to the higher amount of dye adsorption as well as higher photocurrent.</p>
</sec>
<sec>
<st>
<p>Abbreviations</p>
</st>
<p>DI: deionize; DSSCs: dye-sensitized solar cells; TEM: transmission electron microscope; TiCl<sub>4</sub>: titanium tetrachloride; TiO<sub>2</sub>: titanium dioxide; TNA: titanium dioxide nano-tube array; TnB: titanium (IV) n-butoxide; SEM: scanning electron microscopy; XRD: X-ray diffraction.</p>
</sec>
<sec>
<st>
<p>Competing interests</p>
</st>
<p>The authors declare that they have no competing interests.</p>
</sec>
<sec>
<st>
<p>Authors' contributions</p>
</st>
<p>The work presented here was performed in collaboration of all authors. SYH confirmed the results from the preliminary experiments and helped in writing the manuscript. CCC set up the anodization system and carried out the preliminary trails of anodization reaction. CS and WRL discussed the results and wrote the manuscript. SK and CYL proofread the manuscript and corrected the English. All authors read and approved the final manuscript.</p>
</sec>
</bdy><bm>
<ack>
<sec>
<st>
<p>Acknowledgements</p>
</st>
<p>This paper is a revised and expanded version of a paper entitled 'Preparation, characterization and application of titanium nano-tube array in dye-sensitized solar cells' presented at IEEE International NanoElectronics Conference, Taiwan, June 21-24, 2011. We acknowledge the financial support from National Science Council of Taiwan, Republic of China (NSC 98-2113-M-027-003-MY3, NSC 100-2113-M-008-004-MY3).</p>
</sec>
</ack>
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</bm></art>