DOI:
10.1039/C6RA08809K
(Paper)
RSC Adv., 2016,
6, 68997-69006
Electrodeposition of V2O5 on TiO2 nanorod arrays and their electrochromic properties
Received
6th April 2016
, Accepted 29th June 2016
First published on 4th July 2016
Abstract
This paper shows a simple approach for the electrodeposition of V2O5 nanoparticles on a TiO2 nanorod arrays substrate by combining hydrothermal and electrochemical deposition methods. The electrochemical and optical properties of the TiO2/V2O5 hybrid film have been investigated and the results show that the hybrid film has obviously better electrochemical and electrochromic properties compared with the single V2O5 thin film. The TiO2/4cir-V2O5 hybrid film shows the most improved electrochromic properties with excellent cyclic stability, outstanding transmittance modulation (50% at 780 nm) and high coloration efficiency (28 C−1 cm2 at 780 nm). The modified electrochromic properties are mainly due to the TiO2 nanorod array structure, which contributes to improve the structural stability of the V2O5 film and benefits the intercalation/deintercalation process of Li+ ions within the V2O5 film.
1. Introduction
Electrochromism is the reversible and visible change in transmittance and/or reflectance of the films induced by an electrochemical oxidation–reduction reaction.1 The majority of applications of electrochromic devices (ECDs) include: “smart windows” in cars and buildings, reusable price labels and controllable light-reflective or light-transmissive display devices.2,3 In general, a well performed electrochromic film must possess high optical contrast, good optical memory and cyclic stability.4
Many inorganic and organic materials present electrochromism, for inorganic electrochromic materials, especially the transition metal oxides that include oxides of W, V, Mo, Ti (cathodically coloring) and oxides of Ni, Co and Ir (anodically coloring), have attracted a broad interest because of their good performance.5,6
V2O5 has been extensively investigated for its excellent properties like layered structure with high charge capacity,7 good Li+ ion intercalation ability,8 multicolor display9 and low valence vanadium state which leads to easy color changes.10 In addition, V2O5 performs exceptional electrochromic behavior owning to its both anodic and cathodic electrochromism properties.9,11 But there are many disadvantages of using V2O5 films for ECDs: poor cycle reversibility,12 low electrical conductivity and diffusion coefficient of Li+ ions,13 narrow optical modulation and low coloration efficiency.14 Extensive efforts have been dedicated to improve the electrochromic properties of V2O5, such as stability, coloration efficiency, color contrast and reversibility.
A TiO2 electrode with a one-dimensional (1-D) nanorod array has attracted a great deal of attention since its transport properties related to electrons and photons are largely affected by thei one-dimensional geometry.15 Oriented nanorod or nanowire arrays provide a direct pathway for charge transport16 which leads to increased electron diffusion rate,17 and they also provide well-aligned characteristics and high specific surface area.18 Because of these dramatically enhanced properties, nanorod array films of titanium oxide (TiO2) have been widely used in photocatalysis,19,20 dye-sensitized solar cells (DSSCs)17,21 and electrochromic devices (ECDs).22,23
Titanium–vanadium mixed-oxide thin films have been prepared through several methods, such as sol–gel methods,24,25 co-sputtering methods26 and anodization.27 However, reports about the fabrication of TiO2/V2O5 core/shell structure hybrid films are rare. In addition, in our previous investigations we realized that the V2O5 film can be electrodeposited on a rough substrate (NiO nanoporous substrate) more easily than a smooth substrate (ITO), and the electrochromic properties of V2O5 were enhanced effectively. The cycling data showed that NiO/V2O5 composite film exhibits a better reversibility than V2O5 alone. In our new research, we obtained a simple method for preparing the TiO2/V2O5 core/shell structure hybrid film by electrodepositing the V2O5 film on a TiO2 nanorod array substrate (prepared via a hydrothermal method). Also the effect of the underlying TiO2 nanorod array substrate on the electrochromic properties of V2O5 has been studied.
2. Experimental
2.1 Materials
Titanium n-butoxide, concentrated hydrochloric acid, vanadyl sulfate, sodium dodecyl sulfate, sodium chloride, concentrated sulphuric acid, lithium perchlorate, propylene carbonate (PC) and absolute ethyl alcohol were purchased from commercial sources and used without any further purification. FTO coated glass substrates (7 Ω □−1) were purchased and cut into small pieces (2 × 4 cm2 in size) which were cleaned using an ultrasonic method in acetone, ethanol and de-ionized water for 0.5 h, respectively. 1 M nonaqueous solution of LiClO4 in propylene carbonate (PC) was prepared as the electrolyte.
2.2 Preparation of TiO2 nanorod array film
TiO2 nanorod array film has been prepared via hydrothermal method as reported elsewhere.28 The precursor solution was prepared by mixing 15 ml concentrated hydrochloric acid, 15 ml de-ionized water and 0.5 ml titanium n-butoxide in a 100 ml beaker at room temperature. This fresh mixed solution and a clean FTO glass substrate were transferred to a Teflon-lined stainless steel autoclave (45 ml in volume), where FTO substrate was submerged in the solution and placed at an angle against the wall of the Teflon-liner with the conducting side facing down. The hydrothermal synthesis was conducted at 150 °C for 4.5 h in an electric oven. After the synthesis, the FTO substrate was taken out, rinsed extensively with de-ionized water and dried in ambient air. The obtained TiO2 nanorod array films were dried at 80 °C for 12 h and then annealed at 450 °C in air for 0.5 h.
2.3 Preparation of V2O5 film
The V2O5 film was electrodeposited on FTO glass by cyclic voltammetry using a three-electrode system, with Ag/AgCl as the reference electrode, a Pt sheet (1 × 4 cm2) as the counter electrode and FTO glass as the working electrode. The precursor solution was obtained by mixing 1.6 g VOSO4·xH2O as the source of vanadium, 0.1 g sodium dodecyl sulfate as the surfactant and 0.3 g NaCl in a mixed solution of 22.5 ml ethanol and 17.5 ml de-ionized water. The right amount of H2SO4 was added in the solution to keep the pH value in the range of 2–3. Then 4 potential cycle scans were carried out between 0 V and 2.7 V with a rate of 50 mV s−1. After scanning the yellow green film of V2O5 was washed with absolute ethyl alcohol to fully clean up the loosely bounded particles on the surface and then it was dried at 80 °C for 12 h.29
2.4 Preparation of hybrid film of TiO2/V2O5
The hybrid film of TiO2/V2O5 was obtained through the electrodeposition of V2O5 on to the TiO2 nanorod array substrate, which served as the working electrode. This required 1, 4 and 8 potential cycles at a potential between 0 V and 2.7 V with a scanning rate of 50 mV s−1 to prepare the hybrid film of TiO2/V2O5. The hybrid films of TiO2/V2O5 conducted with different potential cycles were named as TiO2/1cir-V2O5, TiO2/4cir-V2O5 and TiO2/8cir-V2O5, respectively. After scanning, the TiO2/V2O5 hybrid films were flushed with absolute ethyl alcohol to wipe off the loosely bounded particles from the films and dried at 80 °C for 12 h.
2.5 Characterization
The structures of the films were tested using X-ray diffraction (SHIMADZU XRD-7000) with Cu Kα radiation. The surface morphologies of the samples were obtained through scanning electron microscopy (SEM, JEOL JSM-7600F). The electrochromic spectra properties were observed with UV-visible absorption spectra, measured using a spectrophotometer (UV-2550, SHIMADZU). The chromaticity was acquired with a spectrophotometer (SP60, X-Rite).
The kinetics of coloration and bleach for the films were measured using a spectrophotometer (UV-2550, SHIMADZU) in cooperation with a CHI660C electrochemical workstation. The step voltages for the V2O5 film and TiO2/V2O5 hybrid film were set up between −0.8 and 1.5 V, and the time for characterization was 20 s. The homemade three-electrode system (platinum wire as the counter electrode, Ag wire as the reference electrode and the electrochromic film on FTO with the size of 0.9 × 3 cm2 as the working electrode) was inserted vertically in the cuvette, which was filled with 1 M LiClO4 in propylene carbonate (PC) as the electrolyte. To insure the light path was unobstructed, the reference electrode and counter electrode were placed on the side of working electrode.
The characteristics of the electrochromic processes were investigated using cyclic voltammetry (CV) and electrochemical impedance spectroscopy (EIS), and the measurements were carried out in a three-electrode system by using a CHI660C electrochemical workstation. A platinum sheet was used as the counter electrode, Ag/AgCl as the reference electrode and 1 M LiClO4 in propylene carbonate (PC) as the electrolyte.
3. Results and discussion
3.1 Morphology and crystalline structure
The crystal structures of the electrochromic films can be confirmed by the investigations of XRD (X-ray diffraction). Fig. 1 illustrates the XRD patterns of FTO, a TiO2 nanorod array film annealed at 450 °C for 0.5 h and the TiO2/V2O5 hybrid films. From Fig. 1b, the annealed TiO2 film reveals diffraction peaks at 36.00°, 41.17°, 50.45°, and 62.66°, which correspond to the (101), (111), (211), and (002) crystal planes of the tetragonal TiO2 phase (JCPDS 21-1276), respectively. It can be seen clearly that the polycrystalline TiO2 film has been prepared successfully through the hydrothermal process and heat treatment. At about 8°, a very important peak of V2O5 appears, which indicates that the V2O5 film has been prepared via electrochemical deposition. As shown in Fig. 1d–f, all the TiO2/V2O5 hybrid films have identical diffraction peaks as shown in Fig. 1c, and this means that V2O5 film has an amorphous structure. In addition, there is a gradual reduction of the peak intensity for TiO2 with the increasing thickness of V2O5. It has been reported that the highly-ordered nanoarray structure is helpful for improving the electrochromic performance and long term stability.30 Thus, this nanoarray TiO2 film can enhance the durability of V2O5 when electrodeposited on the surface of polycrystalline TiO2 nanorod array films.
 |
| Fig. 1 XRD pattern of FTO, annealed TiO2 film, V2O5 film and TiO2/V2O5 hybrid films. | |
Fig. 2 shows the top surface and cross section SEM images of the TiO2 nanorod array film, the V2O5 film and the hybrid films of TiO2/V2O5. As the cross-section morphology shows, the length of the TiO2 nanorods is about 677.8 nm, the thickness of the pure V2O5 film and TiO2/1cir-V2O5, TiO2/4cir-V2O5, and TiO2/8cir-V2O5 hybrid films are 641.3 nm, 816 nm, 998.3 nm and 1.46 μm, respectively. Before the electrodeposition of V2O5 in Fig. 2a, the TiO2 nanorod arrays uniformly cover the surface of the FTO substrate. This intensive film consisted of a large collection of one-dimensional nanorods growing vertically on the substrate. It has been pointed out that one-dimensional nanorod structures generally provide channels for electronic transmission, which are responsible for the diffusion of Li+ ions over short lengths.18 Fig. 2b reveals that V2O5 film were electrodeposited directly on the FTO substrate, which is accumulated by massive nanoparticles with lots of pores on the surface. Compared with the crystalline sample, this amorphous and nanoporous structure is beneficial to intercalate larger amounts of Li+ ions.31 For the TiO2/V2O5 hybrid film (Fig. 2c–e), V2O5 nanoparticles cover the top of the TiO2 nanorod arrays and present an interconnected network structure. With increasing electrodeposition cycles, the porosity of the hybrid film decreased. Clearly, after the TiO2 nanorod array film was electrodeposited with 8 potential cycles, as shown in Fig. 2e, there are few void spaces on the surface of the hybrid film.
 |
| Fig. 2 Surface and cross-section SEM images of (a) V2O5, (b) TiO2, (c) TiO2/1cir-V2O5, (d) TiO2/4cir-V2O5, and (e) TiO2/8-cirV2O5. | |
3.2 Electrochemical and electrochromic properties
The cyclic voltammograms were recorded between −1.0 V and 1.8 V (versus Ag/AgCl) at a scan speed of 50 mV s−1 in a 1 M LiClO4/PC electrolyte to study the electrochemical and electrochromic properties of the films. For the TiO2 nanorod array film (Fig. 3a), there is one pair of redox peaks at −0.46 V and −0.87 V. The cathodic peak is ascribed to Ti4+ reduction coupled with Li+ intercalation, as shown in eqn (1), whereas the anodic peak is assigned to Li+ release.32 |
 | (1) |
 |
| Fig. 3 Cyclic voltammograms of (a) TiO2, (b) V2O5, (c) TiO2/1cir-V2O5, (d) TiO2/4cir-V2O5, and (e) TiO2/8cir-V2O5 films measured in 1 M LiClO4/propylene carbonate. | |
The transition from TiO2 to LixTiO2 after the intercalation and deintercalation of Li+ ions causes the color change of the film in visible range. During the process of the cathodic scan, due to the insertion of Li+ ions, the film becomes colored (light blue). While during the reverse anodic scanning process, the film bleaches (transparent) again following the extraction of Li+ ions.
The V2O5 film (Fig. 3b) shows a completely invertible CV graph where the cathodic peak occurs at −0.4 V, whereas the anodic peak occurs at 0.7 V. Along with the redox peaks, the color of the film changes obviously, blue-gray (at −0.6 V) to green yellow (at 0.6 V) and then green yellow to orange-yellow (at 1.3 V). This was attributed to the injection/extraction of Li+ ions in the V2O5 matrix and can be explained by the following equation:33–35
|
 | (2) |
At the cathodic scanning cycle, a colored vanadium bronze (LixV2O5) was formed caused by the simultaneous intercalation of electrons and Li+ ions into the V2O5 film, and this process made the reduction of pentavalent vanadium (V5+) to its lower valence state (V4+). During the reverse anodic scan, the electrons and Li+ ions were deintercalated out of the V2O5 film leading to the oxidation of lower valence vanadium (V4+) to its pentavalent state (V5+).
As shown in Fig. 3c–e, the hybrid films show similar reduction peaks and oxidation peaks in contrast with the CV of the V2O5 film. This is mainly because the V2O5 layer in the hybrid films plays the main role in the intercalation and deintercalation process of Li+ ions. While the TiO2/4cir-V2O5 hybrid film in Fig. 3d shows a sharp increase in current density in contrast with that of the single V2O5 film, which indicates that the composition of V2O5 with TiO2 nanorod arrays promotes the process of Li+ ion insertion into/extraction from the host lattice. Besides, it can be seen that the current of the film shifts to higher values with the increase of electrodeposition time, which indicates that the amount of Li+ ions and electrons incorporated into the film increases. This is mainly because the film electrode contains more active material with the duration of electrode position.
The cycle life performance of the V2O5 film (Fig. 4a) and TiO2/V2O5 hybrid films (Fig. 4b–d) was studied using 500 cycles with a fixed scan speed of 50 mV s−1. It can be seen in Fig. 4 that the decrease of the current for the TiO2/1cir-V2O5 and TiO2/4cir-V2O5 hybrid films is much smaller than that of the V2O5 film. The result shows that the hybrid films have a more stable electrochemical response up to 500 cycles and good cyclic stability, which suggests the improved performance of V2O5 as an electrochromic material in a hybrid structure for use in ECDs. However, for the TiO2/8cir-V2O5 hybrid film, the current also has a sharp decrease which is similar to Fig. 4a. The reason is that during the cyclic process of the pure V2O5 film, the Li+ ion intercalation/deintercalation capacity of V2O5 decreases with successive charging and discharging cycles, which may be due to an increase in the electrical resistance produced by Li+ ions trapped in structural distortions.36
 |
| Fig. 4 Cyclic voltammograms of (a) V2O5, (b) TiO2/1cir-V2O5, (c) TiO2/4cir-V2O5, and (d) TiO2/8cir-V2O5 films for 500 cycles. | |
3.3 UV-visible transmittance spectra
We further investigated the transmittance modulation and switching response of the electrochromic film through optical transmittance measurements. Fig. 5 shows the optical transmittance spectra of the V2O5 film and TiO2/V2O5 hybrid films in their colored and bleached states under different voltages between 350 nm and 800 nm in 1 M LiClO4/PC electrolyte.
 |
| Fig. 5 Transmittance spectra of (a) V2O5, (b) TiO2/1cir-V2O5, (c) TiO2/4cir-V2O5, (d) TiO2/8cir-V2O5, and (e) TiO2 films at different voltages. | |
As can be seen in Fig. 5a, the transmittance modulation (ΔT = Tb − Tc, Tb and Tc denote transmittance in bleached and colored state) in the wavelength range of 600–800 nm of the V2O5 film is large, with transmittance modulation of 30% at 780 nm. When the wavelength is below 550 nm, the transmittance modulation becomes small. Compared with the transmittance of the V2O5 film, the transmittance of the TiO2/V2O5 hybrid films (Fig. 5b–d) has a similar shift at different voltages. With the increase of the electrodeposition cycle-index of V2O5, the hybrid films become thicker, which leads to the lower Tb and Tc for the TiO2/V2O5 films. However, the TiO2/4cir-V2O5 film has the largest transmittance modulation (50% at 780 nm), as compared to 18% for TiO2/1cir-V2O5 and 45% for TiO2/8cir-V2O5.
3.4 UV-visible absorption spectra
Fig. 6 shows the absorption spectra of the V2O5 film and TiO2/V2O5 hybrid films in the colored and bleached states. Fig. 6a shows that the absorption of the V2O5 film changed obviously depending on whether the film was at a voltage of 1.5 V or −0.8 V. In the bleached state at 1.5 V, a strong absorption occurred in the UV range of 350–400 nm for the V2O5 film. However, the absorption peak appeared around 500 nm in the colored state (−0.8 V). This was mainly caused by the Li+ ions interacting with the film. In the colored state, the absorption peak at long wavelengths was caused by V4+. While in the bleached state, V5+ produced the absorption at short wavelengths. In comparison with the V2O5 film absorption spectra, the TiO2/V2O5 hybrid films show a similar trend but the absorption in the range of 450–350 nm is stronger. This is mainly due to the addition of the TiO2 coated substrate which has a very strong absorption at short wavelengths near the ultraviolet region. Besides, the higher V2O5 electrodeposition cycle-index results in the stronger of absorption of TiO2/V2O5 films obviously.
 |
| Fig. 6 Absorption spectra of (a) V2O5, (b) TiO2/1cir-V2O5, (c) TiO2/4cir-V2O5, (d) TiO2/8cir-V2O5, and (e) TiO2 films at different voltages. | |
3.5 Colorimetry
Colorimetry analysis of the samples can quantitatively define and compare the colors of electrochromic materials. Generally, the color for colorimetric analysis can be represented with three parameters: luminance (L*), hue (a*) and saturation (b*). The relative L*, a* and b* values of the V2O5 film and TiO2/V2O5 hybrid films at different states were measured (Table 1). At the same time, the photos of the films are provided so that the color changes at different states can be observed visually. At 1.5 V, 0.6 V and −0.8 V, the color of the TiO2/V2O5 hybrid films changes from orange yellow (at 1.5 V) to green yellow (at 0.6 V) and blue gray (at −0.8 V). Because the V2O5 layer is the main functional part in the TiO2/V2O5 hybrid films, the hybrid films have no evident change in their color except becoming darker with the thickness of the V2O5 layer increasing.
Table 1 The color parameters and optical images of the V2O5 and TiO2/V2O5 films
Material |
Voltage |
L* |
a* |
b* |
Color |
V2O5 |
1.5 V |
56.56 |
14.86 |
65.84 |
 |
0.6 V |
52.18 |
−9.38 |
38.40 |
 |
−0.8 V |
38.00 |
4.51 |
5.91 |
 |
TiO2/1cir-V2O5 |
1.5 V |
54.04 |
10.31 |
66.16 |
 |
0.6 V |
50.46 |
−10.27 |
35.81 |
 |
−0.8 V |
33.58 |
6.54 |
12.53 |
 |
TiO2/4cir-V2O5 |
1.5 V |
52.75 |
20.64 |
59.34 |
 |
0.6 V |
40.80 |
−6.59 |
33.03 |
 |
−0.8 V |
24.00 |
3.36 |
6.35 |
 |
TiO2/8cir-V2O5 |
1.5 V |
45.02 |
27.93 |
38.16 |
 |
0.6 V |
29.07 |
−3.64 |
10.30 |
 |
−0.8 V |
21.00 |
0.07 |
0.34 |
 |
3.6 Switching speed
Switching speed is one of the major parameters in ECDs and a fast switching speed is necessary for a well-performing ECD. In this paper, switching time is calculated for reaching 90% of the maximum transmittance change between bleached (1.5 V) and colored (−0.8 V) states of the electrochromic film at a wavelength of 780 nm. In order to obtain the switching characteristics of the electrochromic films, chronoamperometry (CA) and the corresponding in situ transmittance measurements were employed. Fig. 7 shows the results of Tb and Tc for the electrochromic films and the switching speeds are listed in Table 2. The TiO2/4cir-V2O5 hybrid film exhibits a faster switching time than other reported electrochromic films based on V2O5.37–40 With the increase of V2O5 deposition time, the switching speed of the TiO2/V2O5 hybrid films becomes slower. In contrast with the switching speed of the V2O5 film, the TiO2/4cir-V2O5 hybrid film has similar coloring and bleaching time. However, the range of change in transmission is much larger for the latter.
 |
| Fig. 7 CA and in situ transmittance curves for (a) V2O5, (b) TiO2/1cir-V2O5, (c) TiO2/4cir-V2O5, and (d) TiO2/8cir-V2O5 films at 780 nm with a voltage interval between −0.8 V (20 s) and 1.5 V (20 s). | |
Table 2 Switching speed of the V2O5 and TiO2/V2O5 thin films
Samples |
Optical modulation range (%) |
Switching speed (s) |
Tb |
Tc |
V2O5 at 780 nm |
30% |
4 |
2 |
TiO2/1cir-V2O5 at 780 nm |
18% |
1 |
1 |
TiO2/4cir-V2O5 at 780 nm |
50% |
3.8 |
3.3 |
TiO2/8cir-V2O5 at 780 nm |
45% |
7 |
3.8 |
3.7 Coloration efficiency
The coloration efficiency (CE) is defined as the ratio of the change in optical density (ΔOD) at a specific wavelength or integrated over a wavelength range to the amount of charge consumed (Q).37 Apparently excellent ECDs should possess a high CE, which means that the largest transmittance change is caused by the least amount of charge. The change in optical density is calculated by using the following formulas,41 where Tb is the bleached transmittance and Tc is the colored transmittance: |
 | (3) |
|
 | (4) |
By combining the chronoamperometry and in situ transmittance versus time test results shown in Fig. 7, the plots of optical density-charge density for the (a) V2O5 film and (b–d) TiO2/V2O5 hybrid films were obtained and shown in Fig. 8. The |CE| value for the V2O5 thin film is 19.3 C−1 cm2 at 780 nm, 21 C−1 cm2 for TiO2/1cir-V2O5, 28 C−1 cm2 for TiO2/4cir-V2O5 and 22 C−1 cm2 for TiO2/8cir-V2O5. The CE of the TiO2/4cir-V2O5 hybrid film is higher than that of the V2O5 film and the other TiO2/V2O5 films. In addition, the CE of the TiO2/4cir-V2O5 hybrid film also shows an improvement compared with the reported electrochromic films based on V2O5.42–45
 |
| Fig. 8 Variation of the in situ optical density (ΔOD) vs. charge density (Q) for (a) V2O5, (b) TiO2/1cir-V2O5, (c) TiO2/4cir-V2O5, and (d) TiO2/8cir-V2O5 films. | |
The enhancement of color efficiency was mainly due to the TiO2 nanorod arrays introduced as a substrate, which thus made for a porous network and high specific surface area of the hybrid films. This structure makes it easier for Li+ ion intercalation and deintercalation in electrochromic films. Besides, the one dimensional TiO2 nanorod arrays have the ability to supply superior electron transport properties.28 All of these promote the charge-transfer reactions of the films in electrochromic processes.
3.8 Electrochemical impedance spectroscopy
To better understand the electrochemical behavior of the V2O5 film and TiO2/V2O5 hybrid films, electrochemical impedance spectroscopy (EIS) was analyzed using three-electrode systems with an AC voltage of 5 mV in a frequency range of 0.01 Hz to 100 kHz in the bleached state (at a polarization of 1.5 V). Ahead of the EIS test, these electrochromic films needed a sufficient activation process with a cyclic voltammetric test for 10 cycles. The Nyquist plots of the V2O5 film and TiO2/V2O5 hybrid films are shown in Fig. 9. The EIS spectra consist of a semicircle which represents the charge-transfer resistance on the interface of the electrode/electrolyte in the high-frequency region and a straight line that attributes to the diffusion of Li+ ions into the bulk of the electrode material in the low frequency region. A larger semicircle means a higher charge-transfer resistance and a lower slope indicates a higher ion-diffusion resistance.22
 |
| Fig. 9 Electrochemical impedance spectroscopy (EIS) of TiO2 film, V2O5 film and TiO2/V2O5 hybrid films recorded in the bleached state. | |
Fig. 9 shows that the semicircle in the high-frequency region for the V2O5 film is larger than that of the TiO2/V2O5 hybrid films in their bleached state, and the TiO2/1cir-V2O5 film has the smallest semicircle. This reveals that the migration resistance and the charge-transfer resistance of Li+ ions for the V2O5 film is larger than that of the TiO2/V2O5 hybrid films. This means the introduction of the TiO2 nanorod array as the substrate provides a higher porosity in the surface and a larger area of the electrode–electrolyte interface,46 leading to an easier migration and charge-transfer process for the Li+ ions at the solid oxide/liquid electrolyte interface. Through simulating the EIS curves, the charge-transfer resistance (Rct) of the pure V2O5 film and TiO2/8cir-V2O5 film is 153.7 Ω and 95.6 Ω, respectively. However, in the low-frequency region, it shows that these films have the almost same slope.
4. Conclusions
In summary, we have synthesized a novel TiO2/V2O5 hybrid film by combining the hydrothermal and electrochemical deposition methods. The electrochemical and optical properties of the TiO2/V2O5 hybrid films have been investigated and it shows the improved electrochemical and electrochromic properties compared with the single V2O5 thin film. The TiO2/4cir-V2O5 hybrid film shows the most improved electrochromic properties with excellent cyclic stability, outstanding transmittance modulation (50% at 780 nm) and high coloration efficiency (28 C−1 cm2 at 780 nm). The modified electrochromic properties are mainly due to the TiO2 nanorod array structure, which contributes to improve the structural stability of the V2O5 film and the intercalation/deintercalation process of Li+ ions within the V2O5 film.
Acknowledgements
We are grateful to the National Natural Science Foundation of China (Grant no. 21572030, 21272033, 21402023) for financial support.
Notes and references
- P. M. S. Monk, R. J. Mortimer and D. R. Rosseinsky, Electrochromism: Fundamentals and Applications, VCH, Weinheim, 1995 Search PubMed.
- P. M. Beaujuge and J. R. Reynolds, Chem. Rev., 2010, 110, 268 CrossRef CAS PubMed.
- E. Koubli, S. Tsakanikas, G. Leftheriotis, G. Syrrokostas and P. Yianoulis, Solid State Ionics, 2015, 272, 30 CrossRef CAS.
- R. J. Mortimer, Chem. Soc. Rev., 1997, 26, 147 RSC.
- Y. Tian, W. Zhang, S. Cong, Y. Zheng, F. Geng and Z. Zhao, Adv. Funct. Mater., 2015, 25, 5833 CrossRef CAS.
- T.-N. Lin, Y. H. Lin, C. T. Lee, S. Han and K.-W. Weng, Thin Solid Films, 2015, 584, 341 CrossRef CAS.
- N. A. Chernova, M. Roppolo, A. C. Dillon and M. S. Whittingham, J. Mater. Chem., 2009, 19, 2526 RSC.
- M. R. J. Scherer, L. Li, P. M. S. Cunha, O. A. Scherman and U. Steiner, Adv. Mater., 2012, 24, 1217 CrossRef CAS PubMed.
- L. Li, U. Steiner and S. Mahajan, J. Mater. Chem., 2010, 20, 7131 RSC.
- M. Najdoski, V. Koleva, S. Stojkovikj and T. Todorovski, Surf. Coat. Technol., 2015, 277, 308 CrossRef CAS.
- C. G. Granqvist, Handbook of Inorganic Electrochromic Materials, Elsevier, New York, 1995 Search PubMed.
- R. Zanoni, F. Decker, C. Coluzza, F. Artuso, N. Cimino, G. Di Santo and E. Masetti, Surf. Interface Anal., 2002, 33, 815–824 CrossRef CAS.
- Z. Tong, N. Li, H. Lv, Y. Tian, H. Qu, X. Zhang, J. Zhao and Y. Li, Sol. Energy Mater. Sol. Cells, 2016, 146, 135 CrossRef CAS.
- Z. Tong, X. Zhang, H. Lv, N. Li, H. Qu, J. Zhao, Y. Li and X.-Y. Liu, Adv. Mater., 2015, 2, 15002301 Search PubMed.
- C. Burda, X. B. Chen, R. Narayanan and M. A. El-Sayed, Chem. Rev., 2005, 105, 1025 CrossRef CAS PubMed.
- H.-L. Feng, W.-Q. Wu, H.-S. Rao, Q. Wan, L.-B. Li, D.-B. Kuang and C.-Y. Su, ACS Appl. Mater. Interfaces, 2015, 7, 5199 CAS.
- Q. Huang, G. Zhou, L. Fang, L. Hu and Z.-S. Wang, Energy Environ. Sci., 2011, 4, 2145–2151 CAS.
- W. Zhou, H. Liu, R. I. Boughton, G. Du, J. Lin, J. Wang and D. Liu, J. Mater. Chem., 2010, 20, 5993 RSC.
- P. Wang, Y. Ao, C. Wang, J. Hou and J. Qian, Mater. Lett., 2013, 101, 41 CrossRef CAS.
- Y. He, P. Basnet, S. E. H. Murph and Y. Zhao, ACS Appl. Mater. Interfaces, 2013, 5, 11818 CAS.
- Y. Chen, Q. Tao, W. Fu, H. Yang, X. Zhou, S. Su, D. Ding, Y. Mu, X. Li and M. Li, Chem. Commun., 2014, 50, 9509 RSC.
- G. F. Cai, D. Zhou, Q. Q. Xiong, J. H. Zhang, X. L. Wang, C. D. Gu and J. P. Tu, Sol. Energy Mater. Sol. Cells, 2013, 117, 231 CrossRef CAS.
- X. Fu, C. Jia, Z. Wan, X. Weng, J. Xie and L. Deng, Org. Electron., 2014, 15, 2702 CrossRef CAS.
- T. Ivanova and A. Harizanova, Mater. Res. Bull., 2005, 40, 411 CrossRef CAS.
- F. Bellenger, C. Chemarin, D. Deroo, S. Maximovitch, A. S. Vuk and B. Orel, Electrochim. Acta, 2001, 46, 2263 CrossRef CAS.
- H. Kakiuchida, P. Jin and M. Tazawa, Thin Solid Films, 2008, 516, 4563 CrossRef CAS.
- Y. Yang, D. Kim and P. Schmuki, Electrochem. Commun., 2011, 13, 1021 CrossRef CAS.
- H. Wang, Y. Bai, Q. Wu, W. Zhou, H. Zhang, J. Li and L. Guo, Phys. Chem. Chem. Phys., 2011, 13, 7008 RSC.
- Y. Liu, C. Jia, Z. Wan, X. Weng, J. Xie and L. Deng, Sol. Energy Mater. Sol. Cells, 2015, 132, 467 CrossRef CAS.
- Y. Yang, D. Kim and P. Schmuki, Electrochem. Commun., 2011, 13, 1198 CrossRef CAS.
- Y. Wang, K. Takahashi, K. Lee and G. Cao, Adv. Funct. Mater., 2006, 16, 1133 CrossRef CAS.
- J.-Z. Chen, W.-Y. Ko, Y.-C. Yen, P.-H. Chen and K.-J. Lin, ACS Nano, 2012, 6, 6633 CrossRef CAS PubMed.
- J. Chu, Z. Kong, D. Lu, W. Zhang, X. Wang, Y. Yu, S. Li, X. Wang, S. Xiong and J. Ma, Mater. Lett., 2016, 166, 179 CrossRef CAS.
- Y.-R. Lu, T.-Z. Wu, C.-L. Chen, D.-H. Wei, J.-L. Chen, W.-C. Chou and C.-L. Dong, Nanoscale Res. Lett., 2015, 10, 1 CrossRef CAS PubMed.
- L. Ottaviano, A. Pennisi, F. Simone and A. M. Salvi, Opt. Mater., 2004, 27, 307 CrossRef CAS.
- M. B. Sahana, C. Sudakar, C. Thapa, V. M. Naik, G. W. Auner, R. Naik and K. R. Padmanabhan, Thin Solid Films, 2009, 517, 6642 CrossRef CAS.
- W. Kang, C. Yan, X. Wang, C. Foo, A. Tan, K. Chee and P. Lee, J. Mater. Chem. C, 2014, 2, 4730 Search PubMed.
- C. Xiong, A. Aliev, B. Gnade and K. Balkus, ACS Nano, 2008, 2, 298 CrossRef PubMed.
- U. Tritschler, F. Beck, H. Schlaad and H. Cölfen, J. Mater. Chem. C, 2015, 3, 952 RSC.
- C. E. Patil, P. R. Jadhav, N. L. Tarwal, H. P. Deshmukh, M. M. Karanjkar and P. S. Patil, Mater. Chem. Phys., 2011, 126, 713 CrossRef.
- M. R. J. Scherer and U. Steiner, Nano Lett., 2013, 13, 3005 CrossRef CAS PubMed.
- W. Kang, C. Yan, X. Wang, C. Foo, A. Tan, K. Chee and P. Lee, J. Mater. Chem. C, 2014, 2, 4730 Search PubMed.
- Z. Tong, N. LI, H. Lv, Y. Tian, H. Qu, X. Zhang, J. Zhao and Y. Li, Sol. Energy Mater. Sol. Cells, 2016, 146, 139 CrossRef.
- R. Oliveira, J. Goulart, F. Miranda and E. Ponzio, J. Braz. Chem. Soc., 2014, 25, 547 Search PubMed.
- C. Patil, N. Tarwal, P. Shinde, H. Deshmukh and P. Patil, J. Phys. D: Appl. Phys., 2009, 42, 025404 CrossRef.
- H. Yu, Y. Li, L. Zhao, G. Li, J. Li, H. Rong and Z. Liu, Mater. Lett., 2016, 169, 65 CrossRef CAS.
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