- Nano Express
- Open Access
CdS/CdSe Co-sensitized Solar Cells Based on Hierarchically Structured SnO2/TiO2 Hybrid Films
© The Author(s). 2016
- Received: 22 January 2016
- Accepted: 23 May 2016
- Published: 14 June 2016
SnO2 nanosheet-structured films were prepared on a fluorine-doped tin oxide (FTO) substrate using ZnO nanosheet as template. The as-prepared SnO2 nanosheets contained plenty of nano-voids and were generally vertical to the substrate. TiO2 nanoparticles were homogeneously deposited into the intervals between the SnO2 nanosheets to prepare a hierarchically structured SnO2/TiO2 hybrid film. The hybrid films were co-sensitized with CdS and CdSe quantum dots. The sensitized solar cells assembled with the SnO2/TiO2 hybrid film showed much higher photoelectricity conversion efficiency than the cells assembled with pure TiO2 films. The lifetime of photoinduced electron was also investigated through electrochemical impedance spectroscopy, which showed that the SnO2/TiO2 hybrid film electrode is as long as the TiO2 film electrode.
- SnO2 nanosheet
- SnO2/TiO2 hybrid films
- Quantum dots
In recent years, quantum dot (QD)-sensitized solar cells have attracted remarkable attention because of the multiple exciton generation characters. The theoretical energy conversion efficiency of QD-sensitized solar cells (QDSCs) was calculated to be about 44.4 % which is much higher than that of the organic dye-sensitized solar cells . Many narrow bandgap semiconductor QDs, such as PbS, CdS, and CdSe, have been extensively used to sensitize TiO2 photoanode [2–5]. Compared with TiO2, SnO2 has many advantages. Firstly, the energy gap of SnO2 is about 3.6 eV which may reduce the effect of UV light in the sunlight on the solar cell performance and improve their long-term stability . Secondly, the electron mobility of SnO2 is about 150 cm2 V−1 s−1 which is much higher than that of TiO2 (1 cm2 V−1 s−1) [7, 8]. Thirdly, SnO2 films which are suitable for sensitized solar cells could be obtained without high temperature calcination [9, 10]. Therefore, some teams began to apply nanoporous SnO2 as photoanodes in QD-sensitized solar cells. Hossain et al. found that TiCl4 treatment can significantly increase the open circuit photovoltage of CdSe QD-sensitized SnO2 solar cells . Then, they co-sensitized SnO2 films with CdS and CdSe QDs and obtained much higher short circuit current (J SC, 17.40 mA cm−2) than that of TiO2 film based QD-sensitized solar cells . Cánovas et al. studied the electron transfer processes from PbSe quantum dots to SnO2 and found that the injection time of the photoexcited electron was vitally affected by the QD size . Xiao et al. found that the shape of SnO2 might affect the photovoltage of SnO2-based QDSCs. They applied highly ordered SnO2 inverse opal films to QDSCs and obtained high open circuit voltage (V OC, 700 mV) and high short circuit current (10.13 mA cm−2). The total photoelectric transfer efficiency was about 4.37 % .
Specific nanostructure of nanoparticles, such as nanorod, nanosheet, and nanowire, could bring some distinctive properties. Some teams had attempted to prepare SnO2 nanosheets. Li Y et al. synthesized SnO2 nanosheets by hydrothermal method from SnCl2 and NaOH in ethanol/water solution . Fei L et al. prepared SnO2 nanosheets using graphite sheets as template . Dong CJ et al. obtained Pt-functionalized SnO2 nanosheets by a facial solution combustion method .
Zinc nitrate hexahydrate (Zn(NO3)2·6H2O), zinc acetate (Zn(CH2COO)2), ammonium hexafluorostannate ((NH4)2SnF6), boric acid (H3BO3), cadmium acetate (Cd(CH2COO)2), selenium powder (Se), sodium thiosulfate (Na2S2O3.5H2O), nitrilotriacetic acid trisodium salt (C6H8NNa3O7), copper nitrate trihydrate (Cu(NO3)2·3H2O), and sodium sulfide (Na2S) were all purchased from Sinopharm Chemical Reagent Co. (SCRC, China). Ethanol and methanol were purchased from Aladdin Reagent Co. (China) with a purity >99.9 %. All of these materials were used as received without any further purification.
The electrodeposition of ZnO nanosheets was carried out in a simple three-electrode glass cell. The precursor solution (for ZnO deposition) consisted of 0.05 M Zn(NO3)2·6H2O and 0.1 M KCl. The working electrode was FTO glass substrates (10 × 10 mm). The reference electrode was Ag/AgCl electrode with saturation potassium chloride aqueous solution, and the counter electrode was Pt metal sheet. The distance between the working electrode and the counter electrode was about 3.5 cm. The deposition temperature was fixed at 70 °C by an oil bath. The deposition potential was controlled to be −1.1 V. The deposition time was controlled to be 30 min unless specially instructed. The deposited samples were cleaned with deionized water, dried at room temperature, and annealed at 450 °C for 30 min in the air atmosphere. The deposition time was controlled to be 30 min. For the formation of SnO2 layer, the ZnO nanosheets were then immersed in a mixture of 3 mL 0.15 mol L−1 (NH4)2SnF6, 1 mL 0.5 mol L−1 H3BO3, and 1 mL deionized water . The immersion time was 4 h to convert all ZnO nanosheets to SnO2 nanosheets. The SnO2 nanosheets were cleaned with deionized water, dried at room temperature, and sintered at 500 °C for 30 min under air atmosphere. Then, the SnO2 nanosheet-structured films were immersed into 40 mM TiCl4 aqueous solution at 70 °C. The immersion time was controlled to be 40 min. The TiCl4-treated SnO2 films were annealed at 500 °C for 30 min under air atmosphere. Then, commercial TiO2 nanoparticles (P25) were deposited on the SnO2 nanosheet through electrophoresis method in a colloid solution (0.5 g P25 dispersed in a mixture of 8 mL butanol, 4 mL isopropanol, and 2 mL ethanol). In the electrophoresis processes, an FTO glass (1 × 2 cm2, 15 Ω sq−1; OPV Tech) was used as the cathode and another FTO glass was used as the anode. The distance between the two electrodes was maintained at 1 cm, and the DC power supply was set at 48 V. The electrophoresis time is 10 s. The SnO2/TiO2 hybrid films were sintered at 500 °C for 30 min.
CdS/CdSe Co-sensitized Photoanodes and Solar Cell Device Fabrication
CdS and CdSe quantum dots were deposited on these nanoporous films (pure SnO2 film, TiCl4-treated SnO2 film, SnO2/TiO2 hybrid film, or pure TiO2 film) in sequence. The deposition process was summarized as follows. Firstly, the nanoporous films were sensitized with CdS quantum dots by successive ionic layer adsorption and reaction (SILAR) method. The deposition process was summarized as follows: (i) The pure ZnO and ZnO/TiO2 composite samples were firstly dipped in the 0.1 M Cd(NO3)2 ethanol solution for 1 min, then rinsed with ethanol for 1 min, followed by dipping in the 0.1 M methanol solution for 1 min and then rinsing with methanol for 1 min. (ii) The former processes were repeated 14 times in order to grow sufficient amount of CdS QDs on the films. Secondly, the CdS-sensitized films were immersed in a mixture of aqueous solution, 0.2 mol L−1 Na2SeSO3, 0.16 mol L−1 C6H8NNa3O7(NTA-3Na), and 0.08 mol L−1 Cd(CH2COO)2 (V:V:V = 1:1:1), for 4 h. Thirdly, the CdS/CdSe co-sensitized films were passivated with ZnS by immersion into 0.1 mol L−1 Zn(CH2COO)2 and 0.1 mol L−1 Na2S aqueous solution in sequence. For QDSCs fabrication, CuS counter electrodes were prepared according to the reported literature . The polysulfide aqueous solution of 1 mol L−1 Na2S, 1 mol L−1 S, and 0.1 mol L−1 NaOH was used as the QDSCs electrolyte.
Measurement and Characterization
The crystalline phase of the samples was characterized by DX-2700 X-ray diffractometer (XRD) with a monochromatized CuK irradiation (k = 0.154145 nm). The morphology was studied using JSM-7001F field emission scanning electron microscope (FE-SEM). Energy dispersive spectroscopy analysis (EDS) was obtained from Bruker-ASX (Model Quan-Tax 200).
The assembled QDSCs were tested under simulated sunlight (AM 1.5G illumination) from a Newport Oriel Solar Simulator (model 94043A, Oriel) using Keithley 2440 Source Meter. The light intensity was calibrated with a standard Si solar cell provided by Newport Oriel. The active cell area of the testing QDSCs was 0.25 cm2. The monochromatic incident photon-to-electron conversion efficiency (IPCE) was measured using an IPCE system (QS 500ADX, Crowntech, Inc.). The testing ranged from 300 to 800 nm. A 150-W tungsten halogen lamp was used as the light source to generate a monochromatic beam. A silicon solar cell was used as the reference during the IPCE measurement. An electrochemistry workstation (IM6) was used to investigate the electrochemical impedance spectra (EIS) of QDSCs. This measurement was also carried out with the same structured QDSCs as that used in the former experiments. The impedance measurement of QDSCs was recorded under dark condition at the bias potential of −0.6 V over a frequency range of 0.1–1 MHz with an AC amplitude of 10 mV.
The conduction band edge of SnO2 is 0.4 V (versus the standard hydrogen electrode (SHE)) which is more positive than that of TiO2. Photoexcited electrons in the conduction band of SnO2 undergo serious back reactions . Coating SnO2 with thin layers of TiO2 is an efficient way to inhibit these back reactions. So the as-prepared SnO2 sheet films were treated in 40 mM TiCl4 aqueous solution at 70 °C for 40 min for the covering of a passivation layer of TiO2. Then, commercial TiO2 nanoparticles (P25) were deposited on the SnO2 sheets through electrophoretic method. Figure 3d shows the cross section of the TiO2 nanoparticle-covered SnO2 film. It can be seen that TiO2 nanoparticles were homogeneously filled in the intervals between SnO2 nanosheets. From the cross section of SnO2/TiO2 hybrid film, the SnO2 nanosheets become so distinct that we can almost not found them. This change of SnO2 might be caused by the mild dissolution of SnO2 in TiCl4 treatment. And the TiO2 nanoparticles were efficiently coated on SnO2 skeleton.
Detailed photovoltaic parameters of the QDSCs obtained from Fig. 5
V OC (mV)
J SC (mA cm−2)
SnO2 + TiCl4
SnO2 + TiCl4 + P25
where J SC is the short circuit photocurrent density at a single wavelength, λ is the wavelength of the incident light, and P in is the power of the incident light. The light absorbed by the photoanodes ranged from 400 nm to about 700 nm which is in accordance with the absorption range of CdS and CdSe. Comparing the curves obtained by different photoanodes, it can be seen that TiCl4 treatment and TiO2 nanoparticle coverage dramatically enhanced the IPCE values during the 400–700 nm, which is in accordance with the results of J-V curves.
The characteristic frequency of these photoanodes, SnO2, TiCl4-treated SnO2, SnO2/TiO2 hybrid film, and pure TiO2 film, were 202.7, 115.4, 1.5, and 1.5 Hz, respectively. According to Eq. 5, the electron lifetimes (τ e) were calculated to be about 0.8, 1.4, and 106.2 ms for the SnO2, TiCl4-treated SnO2, SnO2/TiO2 hybrid film, and TiO2 electrodes, respectively. It can be seen that TiCl4 treatment exactly inhibited the recombination reaction of SnO2 nanosheet electrode. But the effects of TiCl4 treatment are very finite. After the coverage of TiO2, the electron lifetime was lengthened by two orders to the same value as that of the pure TiO2 photoanode. It can be seen that the SnO2/TiO2 hybrid electrode might combine the advantages of both SnO2 nanosheet and TiO2 nanoparticle. This result is in accordance with the J-V curves.
SnO2 nanosheet-structured films were prepared using ZnO nanosheet as template. The as-prepared SnO2 nanosheets contained plenty of nano-voids and were generally vertical to the substrate. TiO2 nanoparticles were homogeneously deposited into the intervals between SnO2 nanosheets to prepare hierarchically structured SnO2/TiO2 hybrid film. The hybrid films were co-sensitized with CdS and CdSe quantum dots. The photoinduced electron showed the same lifetimes in this SnO2/TiO2 hybrid film as that in the pure TiO2 particles films. But the SnO2/TiO2 hybrid film photoanode had higher IPCE than pure TiO2 nanoparticle photoanode. The total photoelectric conversion efficiency was about 3.49 %.
This work was supported by the Natural Science Foundation of China (No. 51304062, 21403056, and U1404202).
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- Hanna MC, Nozik AJ (2006) Solar conversion efficiency of photovoltaic and photoelectrolysis cells with carrier multiplication absorbers. J Appl Phys 100:074510View ArticleGoogle Scholar
- Mu LL, Liu CM, Jia JG, Zhou XW, Lin Y (2013) Dual post-treatment: a strategy towards high efficiency quantum dot sensitized solar cells. J Mater Chem A 1:8353View ArticleGoogle Scholar
- Hyun BR, Zhong YW, Bartnik AC, Sun LF, Abruna HD, Wise FW, Goodreau JD, Matthews JR, Leslie TM, Borrelli NF (2008) Electron injection from colloidal PbS quantum dots into titanium dioxide nanoparticles. ACS Nano 2:2206View ArticleGoogle Scholar
- Zhou R, Niu HH, Zhang QF, Uchaker E, Guo ZQ, Wan L, Miao SD, Xu JZ, Cao GZ (2015) Influence of deposition strategies on CdSe quantum dot-sensitized solar cells: a comparison between successive ionic layer adsorption and reaction and chemical bath deposition. J Mater Chem A 3:12539View ArticleGoogle Scholar
- Yan KY, Chen W, Yang SH (2013) Significantly enhanced open circuit voltage and fill factor of quantum dot sensitized solar cells by linker seeding chemical bath deposition. J Phys Chem C 117:92View ArticleGoogle Scholar
- Senevirathna MKI, Pitigala PK, Premalal EVA, Tennakone K, Kumara GRA, Konno A (2007) Stability of the SnO2/MgO dye-sensitized photo electrochemical solar cell. Sol Energy Mater Sol Cells 91:544View ArticleGoogle Scholar
- Jarzebski ZM, Marton JP (1976) Physical properties of SnO2 materials. 1. Preparation and defect structure. J Electrochem Soc 123:C199View ArticleGoogle Scholar
- Hendry E, Koeberg M, O’Regan B, Bonn M (2006) Local field effects on electron transport in nanostructured TiO2 revealed by terahertz spectroscopy. Nano Lett 6:755View ArticleGoogle Scholar
- Tebby Z, Uddin T, Nicolas Y, Olivier C, Toupance T, Labrugère C, Hirsch L (2011) Low-temperature UV processing of nanoporous SnO2 layers for dye-sensitized solar cells. ACS Appl Mater Interfaces 3:1485View ArticleGoogle Scholar
- Li SJ, Chen Z, Wang YY, Li T, Xu BH, Zhang WF (2014) Flexible photoanode for dye-sensitized solar cells with outstanding short-circuit current based on magnesium oxide-coated tin dioxide films. J Electrochem Soc 161:H1View ArticleGoogle Scholar
- Hossain MA, Yang GW, Parameswaran M, Jennings JR, Wang Q (2010) Mesoporous SnO2 spheres synthesized by electrochemical anodization and their application in CdSe-sensitized solar cells. J Phys Chem C 114:21878View ArticleGoogle Scholar
- Hossain MA, Jennings JR, Koh ZY, Wang Q (2011) Carrier generation and collection in CdS/CdSe-sensitized SnO2 solar cells exhibiting unprecedented photocurrent densities. ACS Nano 5:3172View ArticleGoogle Scholar
- Cánovas E, Moll P, Jensen SA, Gao YN, Houtepen AJ, Siebbeles LSA, Kinge S, Bonn M (2011) Size-dependent electron transfer from PbSe quantum dots to SnO2 monitored by picosecond terahertz spectroscopy. Nano Lett 11:5234View ArticleGoogle Scholar
- Xiao JY, Huang QL, Xu J, Li CH, Chen GP, Luo YH, Li DM, Meng QB (2014) CdS/CdSe co-sensitized solar cells based on a new SnO2 photoanode with a three-dimensionally interconnected ordered porous structure. J Phys Chem C 118:4007View ArticleGoogle Scholar
- Li Y, Guo YQ, Tan RQ, Cui P, Li Y, Song WJ (2013) Synthesis of SnO2 nano-sheets by a template-free hydrothermal method. Mater Lett 63:2085View ArticleGoogle Scholar
- Fei L, Xu Y, Chen Z, Yuan B, Wu XF, Hill JS, Lin QL, Deng SG, Andersen P, Lu YF, Luo HM (2013) Preparation of porous SnO2 helical nanotubes and SnO2 sheets. Mater Chem Phys 140:249View ArticleGoogle Scholar
- Dong CJ, Liu X, Xiao XC, Chen G, Wang YD, Djerdj L (2014) Combustion synthesis of porous Pt-functionalized SnO2 sheets for isopropanol gas detection with a significant enhancement in response. J Mater Chem A 2:20089View ArticleGoogle Scholar
- Desai UV, Xu CK, Wu JM, Gao D (2013) Hybrid TiO2-SnO2 nanotube arrays for dye-sensitized solar cells. J Phys Chem C 117:3232View ArticleGoogle Scholar
- Kalanur SS, Chae SY, Joo OS (2013) Transparent Cu1.8S and CuS thin films on FTO as efficient counter electrode for quantum dot solar cells. Electrochim Acta 103:91View ArticleGoogle Scholar
- Kay A, Grätzel M (2002) Dye-sensitized core-shell nanocrystals: improved efficiency of mesoporous tin oxide electrodes coated with a thin layer of an insulating oxide. Chem Mater 14:2930View ArticleGoogle Scholar
- Tian JJ, Zhang QF, Zhang LL, Gao R, Shen LF, Zhang SG, Qu XH, Cao GZ (2013) ZnO/TiO2 nanocable structured photoelectrodes for CdS/CdSe quantum dot co-sensitized solar cells. Nanoscale 5:936View ArticleGoogle Scholar
- Kern R, Sastrawan R, Ferber J, Stangl R, Luther J (2002) Modeling and interpretation of electrical impedance spectra of dye solar cells operated under open-circuit conditions. Electrochim Acta 47:4213View ArticleGoogle Scholar