Semitransparent inverted polymer solar cells employing a sol-gel-derived TiO2 electron-selective layer on FTO and MoO3/Ag/MoO3 transparent electrode
© Li et al.; licensee Springer. 2014
Received: 2 September 2014
Accepted: 11 October 2014
Published: 17 October 2014
We report a new semitransparent inverted polymer solar cell (PSC) with a structure of glass/FTO/nc-TiO2/P3HT:PCBM/MoO3/Ag/MoO3. Because high-temperature annealing which decreased the conductivity of indium tin oxide (ITO) must be handled in the process of preparation of nanocrystalline titanium oxide (nc-TiO2), we replace glass/ITO with a glass/fluorine-doped tin oxide (FTO) substrate to improve the device performance. The experimental results show that the replacing FTO substrate enhances light transmittance between 400 and 600 nm and does not change sheet resistance after annealing treatment. The dependence of device performances on resistivity, light transmittance, and thickness of the MoO3/Ag/MoO3 film was investigated. High power conversion efficiency (PCE) was achieved for FTO substrate inverted PSCs, which showed about 75% increase compared to our previously reported ITO substrate device at different thicknesses of the MoO3/Ag/MoO3 transparent electrode films illuminated from the FTO side (bottom side) and about 150% increase illuminated from the MoO3/Ag/MoO3 side (top side).
KeywordsPolymer solar cell Indium tin oxide Nanocrystalline titanium oxide Power conversion efficiency
Bulk heterojunction (BHJ) polymer solar cells (PSCs) have been extensively investigated as a new energy substitute due to their low cost, solution processing capability, and flexibility in fabricating large-area devices [1–6]. So far, the power conversion efficiency (PCE) of BHJ PSCs has recently achieved 9.2% or more [7, 8]. It is very close to the commercialization level. However, there are some factors limiting the efficiency of PSCs, such as low absorption efficiency and narrow absorption range, short exciton diffusion length, low charge carrier mobility, and so on [9, 10]. One of the possible strategies to increase its PCE is to stack two or more cells with different spectra response together as tandem solar cells [8, 11]. It is particularly important to study semitransparent solar cells on the investigation of tandem solar cells. Meanwhile, semitransparent BHJ PSCs are also interesting for other applications, such as power-generating windows .
The semitransparent BHJ PSCs require transparent electrodes on both bottom and top sides. There are many researches that focus on top transparent electrodes while the bottom ones typically use indium tin oxide (ITO) electrodes with high transparency in the visible light region [13–18]. And these top transparent electrodes may use one type of thin metal (such as the highly reflective anode Al (100 nm) replaced by a transparent layer of Ag (20 nm) or by a transparent layer of Au (12 nm) [13, 14]), may stack two or more thin metals (such as Al/Au (0.5 nm/15 nm) [15, 16]), or may use multilayer composite structure (such as PEDOT:PSS/PH1000/WO x (40 nm/70 nm/20 nm), WO3/Ag/WO3 (10 nm/13 nm/40 nm) [17, 18]) and so on.
In our previous reports , ITO substrate semitransparent inverted PSCs were studied. The conductivity of ITO decreased because high-temperature (500°C) annealing must be handled during the preparation of nanocrystalline titanium oxide (nc-TiO2). This report focuses on the fluorine-doped tin oxide (FTO) substrate semitransparent inverted PSCs employing a sol-gel-derived TiO2 electron-selective layer (ESL) and with a multilayer anode structure of MoO3/Ag/MoO3. The inner MoO3 layer, which served as a hole transport material (HTM), is inserted between the active layer and Ag to enhance hole collection, and the outer MoO3 layer is used as a top capping layer to enhance light coupling.
The results show that the replacing FTO substrate enhances light transmittance between 400 and 600 nm but does not change sheet resistance after annealing treatment. Compared to our reported ITO substrate inverted PSCs, high PCE about 75% increase was achieved for the FTO substrate device when illuminated from the FTO side (bottom side) and about 150% increase done when illuminated from the MoO3/Ag/MoO3 side (top side).
Current density-voltage (J-V) characteristics were measured using a computer-programmed Keithley 2400 source meter (Keithley 2400, Keithley Instruments, Inc., Cleveland, OH, USA) under AM1.5G solar illumination using a Newport 94043A solar simulator (Newport 94043A, Oriel, Irvine, CA, USA). The intensity of the solar simulator was 100 mW/cm2. Light intensity was corrected by a standard silicon solar cell. The transmission and reflection spectra were measured using ultraviolet/visible (UV-VIS) spectrometer (Carry 5000, Agilent Technologies, Inc., Santa Clara, CA, USA). The resistivity and sheet resistance were measured using four-point probe resistivity measurement (JG SZT-C).
Results and discussion
Characteristic data of semitransparent inverted polymer solar cells
When illuminated from the MoO3/Ag/MoO3 electrode side (top), the efficiency decreases from 2.19% to 1.62% with increasing thickness of MoO3. This phenomenon, which is similar with that of the reported ITO substrate devices (0.96% to 0.60%), might result from the reduced transmittance of MoO3/Ag/MoO3 between 400 and 650 nm when increasing the MoO3 thickness. Figure 2b shows the J-V characteristic curves. The detailed results are given in Table 1. Meanwhile, PCE for FTO substrate inverted PSCs shows about 150% increase compared to the reported ITO substrate. The PCE increases from 0.96% to 2.19%, 0.82% to 1.99%, 0.72% to 1.84%, and 0.60% to 1.64% at MoO3 capping layer thicknesses of 20, 40, 60, and 80 nm, respectively.
One reason of these increases might be that the impact of FTO substrate samples on the environment is reduced, in which the process was in a nitrogen-filled glovebox while the reported process was in the air. The second reason might be that the resistivity of the ITO substrate increases after annealing treatment at high temperature while the resistivity of the FTO substrate does not. For ITO, the oxygen hole as carrier reduction causes the decrease of conductivity after annealing. The third reason might be that the light transmittance of the FTO substrate was a little higher than that of the ITO substrate.
In summary, we demonstrated conductive FTO substrate semitransparent inverted PSCs with high-temperature annealing of nc-TiO2 as an electron-selective layer. The performances of PSCs with different substrates and different thicknesses of the MoO3 capping layer are investigated and compared. As a result, higher PCE was achieved for FTO substrate semitransparent inverted PSCs than that for the ITO substrate both illuminated from the bottom side and from the top side. For structurally identical PSCs, with increasing thickness of the MoO3 capping layer, the PCE is enhanced when illuminated from the bottom side but decreased when illuminated from the top side.
This work was supported by the Science Foundation of Henan University (Grant No. 2013YBZR049), the National Natural Science Foundation of China (Grant No.61306019), the Education Department Foundation of Henan province (Grant No.14A430022), the National Natural Science Foundation of China-Talent Training Fund of Henan (Grant No. U1404616), and Henan University Distinguished Professor Startup Fund.
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