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Article

Perovskite CsPbBr3 Quantum Dots Prepared Using Discarded Lead–Acid Battery Recycled Waste

1
Department of Electro-Optical Engineering, National Taipei University of Technology, Taipei 10608, Taiwan
2
Bachelor Program for Design and Materials for Medical Equipment and Devices, Da-Yeh University, Changhua 51591, Taiwan
3
Department of Electrical Engineering, China University of Science and Technology, Taipei 11581, Taiwan
4
Institute of Advanced Materials and Technology, University of Science and Technology Beijing, Beijing 100083, China
5
Department of Electronic Engineering, Ming Chi University of Technology, New Taipei City 24301, Taiwan
6
Graduate Institute of Optomechatronics Engineering, China University of Science and Technology, Taipei 11581, Taiwan
7
Department of Photonics and Institute of Electro-Optical Engineering, National Chiao Tung University, Hsinchu 30010, Taiwan
8
Department of Chemical Engineering and Materials Science, Yuan Ze University, Taoyuan City 32003, Taiwan
*
Authors to whom correspondence should be addressed.
Energies 2019, 12(6), 1117; https://doi.org/10.3390/en12061117
Submission received: 1 March 2019 / Revised: 17 March 2019 / Accepted: 20 March 2019 / Published: 22 March 2019
(This article belongs to the Special Issue Advanced Quantum Dot Intermediate Band Solar Cells)

Abstract

:
Perovskite CsPbBr3 quantum dot (CsPbBr3-QD) recovery was performed using lead scrap from lead storage batteries. The perovskite CsPbBr3-QD characteristics were analyzed using different PbO/recycled PbO2 ratios. Scanning electron microscopy (SEM) was used to observe the film surface morphology and cross-section. High-resolution transmission electron microscopy (HRTEM) and X-ray diffraction (XRD) were used to observe the perovskite CsPbBr3-QDs’ structural characteristics. A photoluminescence (PL) measurement system was used to analyze the optical properties. The results show that lead scrap from lead–acid batteries as a material for perovskite CsPbBr3-QD production can be successfully synthesized. This saves material and also proves that recycling is valuable. The proposed approach is helpful for future material shortages and materials not easily accessible. Although the efficiency is not very high, this process will be purified using recycled lead in the future to achieve higher quantum yield.

1. Introduction

Organometallic halide perovskite material has special optical and electrical properties due to its unique properties [1,2,3,4]. The diffusion speed of the carrier current is fast, and the diffusion distance is long. The high absorption coefficient has very good absorption in the entire visible light region, and the perovskite material characteristics allow it to fully absorb sunlight during operation and reduce energy loss in the photoelectric conversion process [5,6,7,8]. Perovskite material has a low exciton binding energy, therefore can be excited by light. Organic/inorganic hybrid perovskites, such as MAPbX3 (MA = CH3NH3; X = Cl, Br, I), have attracted widespread attention due to their outstanding performance in solar cells, light-emitting diodes, and optoelectronic devices [9,10,11,12,13,14,15,16,17]. It is worth noting that MAPbI3 has been widely used in the field of solar cells. The power conversion efficiency (PCE) of a perovskite solar cell is up to 23.7% in 2019 [18]. Furthermore, due to band gap tunability (400–800 nm) and narrow emission band of approximately 20 nm, the organic/inorganic hybrid perovskites are considered emission components for phosphor-converted white light-emitting diode (PC-WLED) and electroluminescent (EL) devices in wide-gamut color displays [15,19,20,21]. Compared to organic/inorganic hybrid perovskites, fully inorganic perovskite quantum dots such as CsPbX3 (X = Cl, Br, I) exhibit higher stability and provide excellent thermoelectric performance [22,23,24]. The QD atom arrangement is quite tight and can be used to emit light with different wavelengths using QDs with different sizes due to the quantum confinement effect. QDs are superior to traditional organic dye molecules, because of their brightness, good light stability, and reproducible properties. Therefore, QDs are highly valued in the material chemistry and bio-semiconductor fields [25,26]. This study considers the price of commercial perovskite QDs and the environmental protection problem in preparing perovskite CsPbBr3-QDs at room temperature using waste lead (PbO2) from lead–acid batteries and pure PbO as the Pb-source material. The material and optoelectronic properties of perovskite CsPbBr3-QDs with different ratios of PbO/recycled PbO2 are analyzed and discussed.

2. Materials and Methods

We used scrap lead batteries in this work (standard batteries, 12V). The battery top cover was removed. The acidic electrolyte was poured out and carefully collected. The inner battery wall was rinsed with water several times. Concentrated sulfuric acid (~2.2 M) is contained in the electrolyte and care must be taken to wear protective gloves, safety glasses, and a lab coat during this process. After dismantling the battery, lead source materials (i.e., Pb and PbO2) were washed several times with dilute HCl (35%, Echo Chemical Co., Ltd., Miaoli, Taiwan) and DI water. The resulting anode and cathode were naturally dried under atmospheric conditions. The collected materials were ground into a powder using a mortar and pestle as the recycled PbO2 and ready for the next synthesis.
Recycled PbO2 prepared from a part of the recycled lead–acid battery was mixed with pure PbO (90%, Echo Chemical Co., Ltd., Miaoli, Taiwan). The perovskite QD solution was prepared according to different proportions (in this step we used 100%, 80%, 50%, 20%, and 0% for comparison), and 0.25 mmol Cs2CO3 (99.999%, Echo Chemical Co., Ltd., Miaoli, Taiwan) and 2.5 mL of oleic acid (99%, Echo Chemical Co., Ltd., Miaoli, Taiwan) were added together into a 20 mL glass vial. The mixture was magnetically stirred on a hot plate at 160 °C for 60 min to obtain a clear solution. The glass vial was placed in an oven heated to 120 °C to remove moisture for 30 min, then 2.5 mL of toluene was added to dilute the Cs and Pb precursor solutions to 0.1 M. Next, 1.0 mL of the Cs and Pb precursor solution was decanted into 15 mL of toluene (99%, Echo Chemical Co., Ltd., Miaoli, Taiwan) for 15 min with vigorous stirring while adding 0.05 mmol of Br precursor solution, which was synthesized by tetrabutylammonium bromide (TOAB) (90%, Echo Chemical Co., Ltd., Miaoli, Taiwan), 0.25 mL of oleic acid, and 1.0 mL of toluene. An 8 mL portion of toluene was added to the glass bottle immediately; at this point, a limpid and green CsPbBr3-QD solution was formed. Figure 1 shows the technical procedure for CsPbBr3-QD preparation using recovered waste lead from discarded lead–acid batteries. The deployment ratio is summarized in Table 1.

3. Results and Discussion

Figure 2 shows the X-ray diffraction (XRD) patterns of CsPbBr3-QD films that were deposited onto glass substrates with different PbO/recycled PbO2 ratios. According to a study reports of references [27,28,29], the primary difference between the cubic and orthorhombic crystal structure of CsPbBr3 is a diffraction peak of ~30°. It was illustrated that the two dominant diffraction peaks of the synthesized pure CsPbBr3-QD (PbO(100%):PbO2(0%)) films, namely, (110) at 2θ = 15.193° and (220) at 2θ = 30.739°, demonstrated the cubic perovskite crystal structure. In this work, the structure was similar to those reported in Reference 24. In addition, the few waste lead CsPbBr3-QD (PbO(80%):PbO2(20%), PbO(50%):PbO2(50%), and PbO(20%):PbO2(80%)) films showed weak peaks so that the quantum dots had poor crystallinity and grain aggregation. On the other hand, the waste lead CsPbBr3-QD (PbO(0%):PbO2(100%)) films displayed the three dominant peaks, which were (100) at 2θ = 15.179°, (110) at 2θ = 21.443°, and (200) at 2θ = 30.674°, respectively. It was observed that the (100) diffraction peak intensity was very strong, indicating that CsPbBr3-QDs are high crystallinity along the (100) orientation. The secondary diffraction peak of the (200) plane suggested crystalline perfection. Meantime, the clear splitting of the (100) and (200) diffraction peaks further indicated that the synthesized waste lead CsPbBr3-QD films may be of the room-temperature orthorhombic phase [30].
Figure 3 shows top and cross-sectional scanning electron microscopy (SEM) (GeminiSEM, ZEISS, Oberkochen, Germany) images of CsPbBr3-QDs coated onto indium tin oxide (ITO) glass substrates. It can be clearly seen that there are a large quantity of flakes on the surface of the ITO glass substrate, and each grain size is around 200 nm. Each of them is constructed by the recovered lead perovskite CsPbBr3-QD clusters. This means that the recycled lead perovskite CsPbBr3-QDs can effectively form a thin film. In Figure 3b, it can be seen that the interface is clear and flat. A continuous QD film was formed by stacking CsPbBr3 flakes. The thickness of the recycled lead perovskite CsPbBr3-QDs layered using QD-flake stacking is around 100 nm.
Since the recycled lead perovskite CsPbBr3-QD particle size is very small, it must be clearly examined using high-resolution transmission electron microscopy (HRTEM) to observe the lattice structure of the quantum dots, as well as the quantum dot distribution and particle size. The sample preparation must go through a drying step before examining the quantum dots owing to the inability to observe the QD distribution in the colloidal solution. Therefore, the distribution image is observed using HRTEM, obtained by immersing a copper mesh into the recovered lead perovskite CsPbBr3-QD solution and then drying it by heating. Figure 4 displays the microstructural images observed by TEM (JEM2100F, JEOL, Tokyo, Japan) for CsPbBr3-QD films with different PbO/recycled PbO2 ratios. As shown in Figure 4a, it can be seen that the QD feature clearly presented a nearly cubic shape and good monodispersion in the pure CsPbBr3-QD (PbO(100%):PbO2(0%)) film. However, as the PbO2 content is increased, the QD feature clearly appears in these waste lead CsPbBr3-QD films, as is shown in Figure 4b–e. The average CsPbBr3-QD particle size is evaluated at approximately 10–15 nm. Figure 4f exhibits the high-resolution TEM (HRTEM) image of the waste lead CsPbBr3-QD (PbO(0%):PbO2(100%)) film. The grain with the clear lattice feature can be observed in this image, indicating that it is crystalline. Based on our calculation, the d-spacing value of this lattice arrangement is 2.91 Å, which is indexed to the (200) plane. Except for the HRTEM image, the selected area electron diffraction (SAED) pattern also can be used to confirm the crystal phase. Figure 4g,h shows the SAED images of waste lead CsPbBr3-QD (PbO(50%):PbO2(50%) and PbO(0%):PbO2(100%)) films, respectively. In Figure 4g, the electron diffraction pattern is indistinct, revealing that the CsPbBr3-QD (PbO(50%):PbO2(50%)) film is almost amorphous. On the other hand, the CsPbBr3-QD (PbO(0%):PbO2(100%)) film possesses the clearer electron diffraction pattern. The diffraction rings shown in Figure 4h are determined to be (100) and (200) planes. The TEM observations are in good agreement with the XRD results.
To obtain the CsPbBr3-QDs’ optical properties, the PL spectra for these samples were studied using a fluorescence spectrophotometer system (F-7000, Hitachi, Tokyo, Japan), as shown in Figure 5a. The PL spectral intensity of CsPbBr3-QDs decreases as the PbO2 ratio of waste lead increases. Simultaneously, the PL spectrum shift is usually as a result of the quantum size effect in the nano crystal [31,32]. The pure CsPbBr3-QDs (PbO(100%):PbO2(0%)) and waste lead CsPbBr3-QDs ((PbO(80%):PbO2(20%), PbO(50%):PbO2(50%), PbO(20%):PbO2(80%), and PbO(0%):PbO2(100%)) displayed emission peak positions centered at 488.2, 488.2, 489.6, 493.4, and 483.4 nm, with the narrow full width at half maximum (FWHM) values of 41.48, 43.39, 43.76, 40.83, and 38.32 nm from the PL spectrum, respectively. The photoluminescence quantum yield (PLQY) of all the colloidal CsPbBr3-QDs was estimated to be 40%, as shown in Figure 5b. The PLQY of the CsPbBr3-QDs was lower than that of traditional CsPbBr3-QDs, but the materials in this work were synthesized using used waste lead from discarded lead–acid storage batteries. The perovskite CsPbBr3-QDs prepared using the recycled process in this work save costs and also promote environmental recycling. Future work will involve purifying the recycled lead perovskite CsPbBr3-QDs, increasing the concentration, and promoting PLQY.

4. Conclusions

This study successfully used waste recovered lead oxide from storage batteries as the material to make perovskite CsPbBr3-QDs with different ratios of PbO/recycled PbO2. From the TEM observations, the QD feature clearly appears in these CsPbBr3-QD films. The average CsPbBr3-QD particle size was confirmed using TEM to be approximately 10–15 nm. Based on XRD and TEM results, the CsPbBr3-QD (PbO(0%):PbO2(100%)) film has the higher crystal quality. The CsPbBr3-QD quantum yield was 40% as measured by PLQY. Compared with the price of pure lead or lead oxide as opposed to recycled lead or lead oxide, the current lead recycling can achieve cost savings. However, waste lead recovered from lead storage batteries will exhibit grain agglomeration in the production process. Therefore, it is necessary to optimize the concentration and grain size to improve the quantum yield through a well-designed purification process. Moreover, when the PbO/PbO2 mixture is employed and the PbO2 content increases, and because it is not easy to dissolve PbO2 in oleic acid, a small number of PbO2 particles remain in the mixture, resulting in aggregation of the quantum dots. Therefore, the use of acetic acid or sodium hydroxide as a solvent for PbO2 to improve quantum dot aggregation should be considered in the future.

Author Contributions

L.-C.C. carried out the experiments, designed the study, and gave significant suggestions on the writing of the entire manuscript. C.-H.T. conceived the original idea and wrote the manuscript. S.-L.O. and K.-Y.L. helped to analyze and interpret the data, and helped draft the manuscript. J.T., Z.-L.T., and H.-C.K. reviewed and commented on the manuscript. H.-T.C. prepared the samples and carried out all measurements. A.-C.S. provided HRTEM equipment for image observation. All authors approved this manuscript.

Acknowledgments

This work was supported by the Ministry of Science and Technology (Taiwan) under Contract Nos. 106-2221-E-027-091 and 107-2221-E-027-053, and the NTUT-USTB Joint Research Program under Contract No. NTUT-USTB-107-08.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. Technical procedure for CsPbBr3-QD preparation using recovered waste lead from discarded lead–acid batteries. (a) Discarded lead–acid battery, (b) Electrode inside battery, (c) Recycled electrodes (PbO2 anode and Pb cathode), (d) Grinding PbO2, (e) Collected PbO2 powder, and (f) CsPbBr3-QDs with different ratios under UV-365 nm laser excitation (left to right: PbO/recycled PbO2 ratio = 100%, 80%, 5%, 20%, and 0%).
Figure 1. Technical procedure for CsPbBr3-QD preparation using recovered waste lead from discarded lead–acid batteries. (a) Discarded lead–acid battery, (b) Electrode inside battery, (c) Recycled electrodes (PbO2 anode and Pb cathode), (d) Grinding PbO2, (e) Collected PbO2 powder, and (f) CsPbBr3-QDs with different ratios under UV-365 nm laser excitation (left to right: PbO/recycled PbO2 ratio = 100%, 80%, 5%, 20%, and 0%).
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Figure 2. X-ray diffraction (XRD) patterns of CsPbBr3-QD films with different PbO/recycled PbO2 ratios.
Figure 2. X-ray diffraction (XRD) patterns of CsPbBr3-QD films with different PbO/recycled PbO2 ratios.
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Figure 3. (a) Top and (b) cross-sectional scanning electron microscopy (SEM) images of CsPbBr3-QDs on ITO glass substrate.
Figure 3. (a) Top and (b) cross-sectional scanning electron microscopy (SEM) images of CsPbBr3-QDs on ITO glass substrate.
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Figure 4. TEM images of CsPbBr3-QD films with (a) PbO(100%):PbO2(0%), (b) PbO(80%):PbO2(20%), (c) PbO(50%):PbO2(50%), (d) PbO(20%):PbO2(80%), and (e) PbO(0%):PbO2(100%) ratios. (f) HRTEM image of the CsPbBr3-QD (PbO(0%):PbO2(100%)) film. SAED images of CsPbBr3-QD films with (g) PbO(50%):PbO2(50%) and (h) PbO(0%):PbO2(100%) ratios.
Figure 4. TEM images of CsPbBr3-QD films with (a) PbO(100%):PbO2(0%), (b) PbO(80%):PbO2(20%), (c) PbO(50%):PbO2(50%), (d) PbO(20%):PbO2(80%), and (e) PbO(0%):PbO2(100%) ratios. (f) HRTEM image of the CsPbBr3-QD (PbO(0%):PbO2(100%)) film. SAED images of CsPbBr3-QD films with (g) PbO(50%):PbO2(50%) and (h) PbO(0%):PbO2(100%) ratios.
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Figure 5. (a) Photoluminescence (PL) spectra of CsPbBr3-QD solutions with different PbO/recycled PbO2 ratios; (b) photoluminescence quantum yield (PLQY) of CsPbBr3-QDs.
Figure 5. (a) Photoluminescence (PL) spectra of CsPbBr3-QD solutions with different PbO/recycled PbO2 ratios; (b) photoluminescence quantum yield (PLQY) of CsPbBr3-QDs.
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Table 1. The CsPbBr3-QD deployment ratio in this work.
Table 1. The CsPbBr3-QD deployment ratio in this work.
PbO/Recycled PbO2 RatioCs2CO3PbORecycled PbO2
100%81.45 mg0 mg113.60 mg
80%81.45 m g22.32 mg89.28 mg
50%81.45 mg55.80 mg55.80 mg
20%81.45 mg89.28 mg22.32 mg
0%81.45 mg113.60 mg0 mg

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MDPI and ACS Style

Chen, L.-C.; Tien, C.-H.; Ou, S.-L.; Lee, K.-Y.; Tian, J.; Tseng, Z.-L.; Chen, H.-T.; Kuo, H.-C.; Sun, A.-C. Perovskite CsPbBr3 Quantum Dots Prepared Using Discarded Lead–Acid Battery Recycled Waste. Energies 2019, 12, 1117. https://doi.org/10.3390/en12061117

AMA Style

Chen L-C, Tien C-H, Ou S-L, Lee K-Y, Tian J, Tseng Z-L, Chen H-T, Kuo H-C, Sun A-C. Perovskite CsPbBr3 Quantum Dots Prepared Using Discarded Lead–Acid Battery Recycled Waste. Energies. 2019; 12(6):1117. https://doi.org/10.3390/en12061117

Chicago/Turabian Style

Chen, Lung-Chien, Ching-Ho Tien, Sin-Liang Ou, Kun-Yi Lee, Jianjun Tian, Zong-Liang Tseng, Hao-Tian Chen, Hao-Chung Kuo, and An-Cheng Sun. 2019. "Perovskite CsPbBr3 Quantum Dots Prepared Using Discarded Lead–Acid Battery Recycled Waste" Energies 12, no. 6: 1117. https://doi.org/10.3390/en12061117

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