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Integrating Ultrathin Bulk‐Heterojunction Organic Semiconductor Intermediary for High‐Performance Low‐Bandgap Perovskite Solar Cells with Low Energy Loss
[ASAP] Effects of Moisture-Based Grain Boundary Passivation on Cell Performance and Ionic Migration in Organic–Inorganic Halide Perovskite Solar Cells
[ASAP] Layered Mixed Tin–Lead Hybrid Perovskite Solar Cells with High Stability

Interfacial engineering enables high efficiency with a high open-circuit voltage above 1.23 V in 2D perovskite solar cells
DOI: 10.1039/C8TA06925E, Paper
High efficiency (12.07%) 2D perovskite solar cells with a high open-circuit voltage above 1.23 V are realized via interface engineering.
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Regulating the electron transporting properties of indacenodithiophene derivatives for perovskite solar cells with PCEs up to 19.51%
DOI: 10.1039/C8TA06730A, Paper
ITCPTC as an ETL provides PSCs with an efficiency of 17.42% and as an interlayer offers a remarkable efficiency of 19.51%.
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Temperature-assisted crystallization for inorganic CsPbI2Br perovskite solar cells to attain high stabilized efficiency 14.81%
Publication date: October 2018
Source: Nano Energy, Volume 52
Author(s): Dongliang Bai, Hui Bian, Zhiwen Jin, Haoran Wang, Lina Meng, Qian Wang, Shengzhong (Frank) Liu
Abstract
Due to its super thermal stability, inorganic CsPbI2Br perovskite has attracted more and more attention in the field of photovoltaic application. However, its device performance, as reported to date, is greatly challenged in preparing CsPbI2Br films with both sufficient absorbance and high quality. Herein, crystallization engineering is applied in producing solution-processed CsPbI2Br film to guarantee sufficient light harvesting and effective carrier extraction. Further study proves that the precursor solution temperature would largely affect the crystallization progress: (1) the nucleation step is highly related to the solubility of precursor in a specific solvent or solvents at elevated temperatures; (2) the crystal growth rate is highly related to the solvent evaporation rate. To obtain thick film with larger crystalline grain size, the precursor solution temperature should be carefully adjusted for both suppressing the formation of too many nuclei and increasing the crystallization rate at the same time. Finally, the optimized CsPbI2Br would be obtained when the precursor solution is maintained at 100 °C, the corresponding device shows a stabilized efficiency as high as 14.81%. As far as we know, this is the highest PCE for the CsPbBrI2 perovskite based solar cells.
Graphical abstract
Herein, the correlation between crystallization and external factors (solubility and solvent evaporation rate) is conducted for solution-processed CsPbI2Br film. With moderate precursor solution temperature, homogenous, pinhole-free, large crystalline grain size and thick CsPbI2Br film was obtained, which effectively increased the light absorption, and decreased recombination loss. As a result, the optimized champion device achieved long-term stabilized PCE of 14.81%.
Solvent Engineering to Balance Light Absorbance and Transmittance in Perovskite for Tandem Solar Cells
Through adjusting volume ratios between N‐dimethyl formamide and dimethyl sulfoxide, light absorbance and transmittance of perovskite films in tandem devices is up to balance. The effect of different solvents on surface structure and the photoelectric properties of FACs perovskite materials are systematically examined. The solvent engineering is further extended to a more complicated FAMACs perovskite/SHJ by delivering an optimal power conversion efficiency of 22.80%.
Owing to their rational distribution and adequate use of the solar spectrum and a high open‐circuit voltage, perovskite/silicon‐heterojunction (SHJ) tandem solar cells can exceed the theoretical limit of efficiency for crystalline silicon solar cells. To improve the performance of perovskite/SHJ tandem solar cells, the distribution of the solar spectrum and current matching between sub‐cells must be examined and optimized. This study employs mixed perovskite as the top cell, which is prepared with pure N, N‐dimethyl formamide (DMF), pure dimethyl sulfoxide (DMSO), and mixtures of these components in different volume ratios. The effect of different solvents on surface structure and the photoelectric properties of FACs perovskite materials are systematically examined. When the volume fraction of DMSO is 40%, a smooth, well passivated, high‐quality perovskite film is obtained. Most importantly, light absorbance and transmittance are balanced by applying solvent engineering to optimize perovskite films in the tandem devices. This method can be further extended to a more complicated FAMACs perovskite/SHJ by delivering a power conversion efficiency of 22.80%. This study concludes that solvent engineering is an effective and simple method for modifying the performance of monolithic perovskite/silicon tandem devices.
Versatility of Carbon Enables All Carbon Based Perovskite Solar Cells to Achieve High Efficiency and High Stability
Tris(8‐hydroxyquinoline)aluminum(III)‐Cored Molecular Cathode Interlayer: Improving Electron Mobility and Photovoltaic Efficiency of Polymer Solar Cells
A series of tris(8‐hydroxyquinoline)aluminum(III) (Alq3)‐cored small molecular electrolytes, Alq3‐F1, Alq3‐F2, and Alq3‐F3, armed with ammonium functionalized fluorene units have been successfully designed and synthesized as efficient cathode interlayers (CILs) for high‐performance fullerene and non‐fullerene polymer solar cells (F‐PSCs and NF‐PSCs). The proportion of account of Alq3 segment will balance the conductivity and interfacial modification ability, whose devices exhibit the highest power conversion efficiencies (PCEs) of 10.15% in F‐PSCs and 13.75% in NF‐PSCs. Importantly, these CIL molecules have the excellent thickness‐insensitive property enabled by high electron mobility of the Alq3 core. The PCEs of the PSCs incorporating the Alq3‐containing CILs can retain about 70–80% even with a large thickness up to 50 nm.
Tris(8‐hydroxyquinoline)aluminum(III) (Alq3)‐cored small molecular electrolytes, Alq3‐F1, Alq3‐F2, and Alq3‐F3, armed with ammonium functionalized fluorene units have been successfully designed and synthesized as efficient cathode interlayers (CILs) for high‐performance fullerene and non‐fullerene polymer solar cells (F‐PSCs and NF‐PSCs). The repeating number effect of the polar group‐grafted fluorene arms is also investigated in detail on the cathode interfacial modification and the final photovoltaic performance. Increasing the amount of ammonium functionalized fluorene units will efficiently improve the interfacial dipole moment and result in lowering the work function (W F) of the Al cathode. On the other hand, the proportion of Alq3 segment will decrease with increasing the repeating number of the polar group‐grafted fluorene arms, which deduce the electron mobility of the target molecules. Alq3‐F2 shows a good balance between the above two factors, whose devices exhibit the highest power conversion efficiencies (PCEs) of 10.15% in F‐PSCs and 13.75% in NF‐PSCs. Importantly, these CIL molecules have the excellent thickness‐insensitive property enabled by the high electron mobility of the Alq3 core. The PCEs of the PSCs incorporating the Alq3‐containing CILs can retain about 70–80% even with a large thickness up to 50 nm.
Polymer Assisted Small Molecule Hole Transport Layers Toward Highly Efficient Inverted Perovskite Solar Cells
The hole extraction property of the hole transport layer based on TAPC small molecule via polymer assistance is largely improved. The average power conversion efficiency is enhanced from 17.66 ± 0.52% to 19.03 ± 0.53%, and the champion efficiency reaches 21.01%.
In this paper, inverted perovskite solar cells (PSCs) employing a novel polymer‐assisted small molecule layer as hole transport layer (HTL) are reported and the effect of mixed HTL on the device performance is investigated. It is the first time that the small molecule HTL is doped with a polymer HTL. The introduction of appropriate content of polymer into the small molecule layer will lead to a much smoother surface for the mixed HTL and largely reduced charge recombination, and most importantly, the energy level alignment is more matched with that of the perovskite via optimization of the doping content. Therefore, the hole transfer property is largely improved for the perovskite/mixed HTL composites. After the optimization of the polymer content in the mixed HTLs, an average power conversion efficiency (PCE) of 19.03 ± 0.53% is achieved, and the champion device exhibits a PCE of >21%. This work provides an effective strategy for the development of highly efficient inverted PSCs based on small molecule HTLs.
[ASAP] Enhancing Efficiency and Stability of Perovskite Solar Cells via a Self-Assembled Dopamine Interfacial Layer
[ASAP] Efficiently Improving the Stability of Inverted Perovskite Solar Cells by Employing Polyethylenimine-Modified Carbon Nanotubes as Electrodes
[ASAP] All-Solution-Processed Thermally and Chemically Stable Copper–Nickel Core–Shell Nanowire-Based Composite Window Electrodes for Perovskite Solar Cells
The thermodynamics and kinetics of iodine vacancies in the hybrid perovskite methylammonium lead iodide
DOI: 10.1039/C8EE01697F, Paper
A quantitative description of the ionic conductivity of MAPbI3 is built on two pillars: knowledge of the iodine-vacancy jump rate and of the density of iodine defects.
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Polymer Assisted Small Molecule Hole Transport Layers Toward Highly Efficient Inverted Perovskite Solar Cells
The hole extraction property of the hole transport layer based on TAPC small molecule via polymer assistance is largely improved. The average power conversion efficiency is enhanced from 17.66 ± 0.52% to 19.03 ± 0.53%, and the champion efficiency reaches 21.01%.
In this paper, inverted perovskite solar cells (PSCs) employing a novel polymer‐assisted small molecule layer as hole transport layer (HTL) are reported and the effect of mixed HTL on the device performance is investigated. It is the first time that the small molecule HTL is doped with a polymer HTL. The introduction of appropriate content of polymer into the small molecule layer will lead to a much smoother surface for the mixed HTL and largely reduced charge recombination, and most importantly, the energy level alignment is more matched with that of the perovskite via optimization of the doping content. Therefore, the hole transfer property is largely improved for the perovskite/mixed HTL composites. After the optimization of the polymer content in the mixed HTLs, an average power conversion efficiency (PCE) of 19.03 ± 0.53% is achieved, and the champion device exhibits a PCE of >21%. This work provides an effective strategy for the development of highly efficient inverted PSCs based on small molecule HTLs.
Tris(8‐hydroxyquinoline)aluminum(III)‐Cored Molecular Cathode Interlayer: Improving Electron Mobility and Photovoltaic Efficiency of Polymer Solar Cells
A series of tris(8‐hydroxyquinoline)aluminum(III) (Alq3)‐cored small molecular electrolytes, Alq3‐F1, Alq3‐F2, and Alq3‐F3, armed with ammonium functionalized fluorene units have been successfully designed and synthesized as efficient cathode interlayers (CILs) for high‐performance fullerene and non‐fullerene polymer solar cells (F‐PSCs and NF‐PSCs). The proportion of account of Alq3 segment will balance the conductivity and interfacial modification ability, whose devices exhibit the highest power conversion efficiencies (PCEs) of 10.15% in F‐PSCs and 13.75% in NF‐PSCs. Importantly, these CIL molecules have the excellent thickness‐insensitive property enabled by high electron mobility of the Alq3 core. The PCEs of the PSCs incorporating the Alq3‐containing CILs can retain about 70–80% even with a large thickness up to 50 nm.
Tris(8‐hydroxyquinoline)aluminum(III) (Alq3)‐cored small molecular electrolytes, Alq3‐F1, Alq3‐F2, and Alq3‐F3, armed with ammonium functionalized fluorene units have been successfully designed and synthesized as efficient cathode interlayers (CILs) for high‐performance fullerene and non‐fullerene polymer solar cells (F‐PSCs and NF‐PSCs). The repeating number effect of the polar group‐grafted fluorene arms is also investigated in detail on the cathode interfacial modification and the final photovoltaic performance. Increasing the amount of ammonium functionalized fluorene units will efficiently improve the interfacial dipole moment and result in lowering the work function (W F) of the Al cathode. On the other hand, the proportion of Alq3 segment will decrease with increasing the repeating number of the polar group‐grafted fluorene arms, which deduce the electron mobility of the target molecules. Alq3‐F2 shows a good balance between the above two factors, whose devices exhibit the highest power conversion efficiencies (PCEs) of 10.15% in F‐PSCs and 13.75% in NF‐PSCs. Importantly, these CIL molecules have the excellent thickness‐insensitive property enabled by the high electron mobility of the Alq3 core. The PCEs of the PSCs incorporating the Alq3‐containing CILs can retain about 70–80% even with a large thickness up to 50 nm.
[ASAP] Polar Solvent Induced Lattice Distortion of Cubic CsPbI3 Nanocubes and Hierarchical Self-Assembly into Orthorhombic Single-Crystalline Nanowires
Polymer Donors for High‐Performance Non‐Fullerene Organic Solar Cells
Polymer power: Polymer donors have shown remarkable photovoltaic performance in non‐fullerene organic solar cells (OSCs). The molecular design strategies are analyzed in terms of developing suitable polymer donors for non‐fullerene acceptors to further improve the power conversion efficiency (PCE) of non‐fullerene organic solar cells.
Abstract
Over the past few years, non‐fullerene organic solar cells have been a focus of research and their power conversion efficiencies have been improved dramatically from about 6 % to over 14 %. In addition to innovations in non‐fullerene acceptors, the ongoing development of polymer donors has contributed significantly to the rapid progress of non‐fullerene organic solar cell performance. This Minireview highlights the polymer donors that enable high‐performance non‐fullerene organic solar cells. We show the impressive photovoltaic devices results achieved by some of important classes of conjugated polymer systems in non‐fullerene organic solar cells. We discuss the molecular design strategies as far as developing matching polymer donors for non‐fullerene acceptors. We conclude with a brief summary and outlook for advances in donor polymers required for commercialization.
Resolving Hysteresis in Perovskite Solar Cells with Rapid Flame‐Processed Cobalt‐Doped TiO2
Giant barocaloric tunability in [(CH3CH2CH2)4N]Cd[N(CN)2]3 hybrid perovskite
DOI: 10.1039/C7TC03136J, Paper
[TPrA]Cd[dca]3 shows giant barocaloric tunability and large barocaloric effect, which are desirable for future low-pressure barocaloric cooling applications.
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[ASAP] Halide-, Hybrid-, and Perovskite-Functionalized Light Absorbing Quantum Materials of p–i–n Heterojunction Solar Cells
[ASAP] Performance Enhancement of Mesoporous TiO2-Based Perovskite Solar Cells by SbI3 Interfacial Modification Layer
[ASAP] Water-Repellent Low-Dimensional Fluorous Perovskite as Interfacial Coating for 20% Efficient Solar Cells
Planar Metasurfaces Enable High‐Efficiency Colored Perovskite Solar Cells
A type of macroscopic planar metasurface absorber with light near‐perfectly and exclusively absorbed by the ultrathin semiconductor film is theoretically and experimentally demonstrated via a general strategy. Guided by this strategy, colored perovskite solar cells are further designed to meet all the desired characteristics including high power conversion efficiency, high‐purity, tunability, and angle‐insensitive colors.
Abstract
The achievement of perfect light absorption in ultrathin semiconductor materials is not only a long‐standing goal, but also a critical challenge for solar energy applications, and thus requires a redesigned strategy. Here, a general strategy is demonstrated both theoretically and experimentally to create a planar metasurface absorber comprising a 1D ultrathin planar semiconductor film (replacing the 2D array of subwavelength elements in classical metasurfaces), a transparent spacer, and a metallic back reflector. Guided by derived formulisms, a new type of macroscopic planar metasurface absorber is experimentally demonstrated with light near‐perfectly and exclusively absorbed by the ultrathin semiconductor film. To demonstrate the power and simplicity of this strategy, a prototype of a planar metasurface solar cell is experimentally demonstrated. Furthermore, the device model predicts that a colored planar metasurface perovskite solar cell can maintain 75% of the efficiency of its black counterpart despite the use of a perovskite film that is one order of magnitude thinner. The displayed cell colors have high purities comparable to those of state‐of‐the‐art color filters, and are insensitive to viewing angles up to 60°. The general theoretical framework in conjunction with experimental demonstrations lays the foundation for designing miniaturized, planar, and multifunctional solar cells and optoelectronic devices.
Solar Cells: Enhancing the Performance of the Half Tin and Half Lead Perovskite Solar Cells by Suppression of the Bulk and Interfacial Charge Recombination (Adv. Mater. 35/2018)
All-inorganic perovskite nanocrystal scintillators
All-inorganic perovskite nanocrystal scintillators
All-inorganic perovskite nanocrystal scintillators, Published online: 27 August 2018; doi:10.1038/s41586-018-0451-1
All-inorganic perovskite nanocrystals containing caesium and lead provide low-cost, flexible and solution-processable scintillators that are highly sensitive to X-ray irradiation and emit radioluminescence that is colour-tunable across the visible spectrum.Transformation from crystalline precursor to perovskite in PbCl2-derived MAPbI3
Transformation from crystalline precursor to perovskite in PbCl2-derived MAPbI3
Transformation from crystalline precursor to perovskite in PbCl<sub>2</sub>-derived MAPbI<sub>3</sub>, Published online: 27 August 2018; doi:10.1038/s41467-018-05937-4
The existence of a crystalline precursor is key to perovskite film formation, but the precise chemistry of the precursor and its transformation into perovskite are poorly understood. Here, the authors identify the crystal structure and conversion chemistry of the precursor for PbCl2-derived methylammonium lead iodide perovskites.[ASAP] Ultrafast Intraband Spectroscopy of Hot-Carrier Cooling in Lead-Halide Perovskites

State‐of‐the‐Art Electron‐Selective Contacts in Perovskite Solar Cells
Electron‐selective contacts (ESLs) with tailored properties show improved device performance in both mesoporous and planar perovskite solar cells. The recent development of metal oxide and organic molecules as ESLs is summarized. Understanding the role of various ESLs in different device architectures is a key to achieve high efficiency and long‐term stability.
Abstract
Perovskite solar cells (PSCs) have attracted much attention as efficiencies go beyond 22%. To achieve these impressive numbers, the PSC scientific community is working to improve both the perovskite optoelectronic properties, and, importantly, the interfacial properties of the adjacent electron selective contacts (ESLs). Improvements in both fronts have happened concurrently and are responsible for these rapid efficiency gains. Here, the authors review the recent advances in understanding the role of ESLs on performance improvements. ESLs can be prepared from either organic and inorganic semiconductors, or a combination of both, and their key characteristics are summarized in detail. Current state‐of‐the‐art PSCs employ fully inorganic ESLs made of a thin mesoporous TiO2 or a planar SnO2, with reported certified efficiencies of 22.7 and 20.9%, respectively. While TiO2 shows excellent performance in the short term, it has also been shown to induce solar cell degradation due to its UV absorption properties. Understanding ESLs has been instrumental in the rapid development of PSCs; however, some challenges remain in terms of understanding the role of different ESLs on the long‐term stability of the devices.
Enhancement of the Interfacial Connection via Carboxyl‐Substituted Perylene as Electron‐Transport Layer for Efficient and Stable Perovskite Solar Cells
Carboxyl‐substituted perylene (PTCA) has been successfully applied as the electron‐transport layer in perovskite solar cells. By the carboxyl groups, PTCA can effectively connect the perovskite layer and FTO, thus reducing the interface barriers induced by weak contact, resulting in a high PCE of 16.09%. In addition, the PTCA‐based devices exhibit remarkable stability under illumination in ambient conditions without encapsulation.
Carboxyl‐substituted perylene (PTCA) has been successfully applied as the electron‐transport layer in perovskite solar cells. The large rigid π–π conjugated plane structure in PTCA endows it excellent electronic transmission performance. By the carboxyl groups, PTCA can effectively connect the perovskite layer and FTO, thus reducing the interface barriers induced by weak contact, resulting in a high PCE of 16.09%. In addition, the PTCA‐based devices exhibit remarkable stability under illumination in ambient conditions without encapsulation.







