TY - GEN A1 - Das, Chittaranjan A1 - Kedia, Mayank A1 - Zuo, Weiwei A1 - Mortan, Claudiu A1 - Kot, Małgorzata A1 - Flege, Jan Ingo A1 - Saliba, Michael T1 - Band Bending at Hole Transporting Layer-Perovskite Interfaces in n-i-p and in p-i-n Architecture T2 - Solar RRL N2 - Interfaces between hybrid perovskite absorber and its adjacent charge-transporting layers are of high importance for solar cells performance. Understanding their chemical and electronic properties is a key step in designing efficient and stable perovskite solar cells. In this work, the tapered cross-section photoemission spectroscopy (TCS-PES) method is used to study the methylammonium lead iodide (CH3NH3PbI3) (MAPI)-based solar cells in two configurations, that is, in an inverted p–i–n and in a classical n–i–p architecture. It is revealed in the results that the MAPI film deposited once on the n-type TiO2 and once on the p-type NiOx substrates is neither an intrinsic semiconductor nor adapts to the dopant nature of the substrate underneath, but it is heavily n-type doped on both substrates. In addition to that, the TCS-PES results identify that the band bending between the MAPI film and the hole transporting layer (HTL) layer depends on the perovskite solar cells architecture. In particular, a band bending on the HTL side in the n–i–p and at the MAPI in the p–i–n architecture is found. The flat band of NiOx at the NiOx/MAPI interface can be explained by the Fermi level pinning of the NiOx at the interface. KW - band bending KW - hole transporting layer KW - perovskites KW - X-ray photoelectron spectroscopy (XPS) Y1 - 2022 U6 - https://doi.org/10.1002/solr.202200348 SN - 2367-198X VL - 6 IS - 9 ER - TY - GEN A1 - Zia, Waqas A1 - Malekshahi Byranvand, Mahdi A1 - Rudolph, Toby A1 - Rai, Monika A1 - Kot, Małgorzata A1 - Das, Chittaranjan A1 - Kedia, Mayank A1 - Zohdi, Mohammadreza A1 - Zuo, Weiwei A1 - Yeddu, Vishal A1 - Saidaminov, Makhsud I. A1 - Flege, Jan Ingo A1 - Kirchartz, Thomas A1 - Saliba, Michael T1 - MAPbCl3 Light Absorber for Highest Voltage Perovskite Solar Cells T2 - ACS Energy Letters N2 - Perovskite solar cells (PSCs) excel in achieving high open-circuit voltages (VOC) for narrow bandgaps (∼1.6 eV) but face challenges with wide-bandgap perovskites, like methylammonium lead trichloride (MAPbCl3) with a 3.03 eV bandgap. These materials are transparent in visible absorbing ultraviolet (UV) light. However, achieving uniform film crystallization remains a hurdle. Here, we enhance MAPbCl3 crystallization by manipulating annealing atmospheres (nitrogen, air, and MACl vapor). Excess MACl vapor improves surface coverage, which is crucial for film stability. We demonstrate that the microstructure of the perovskite film, including surface morphology, grain boundaries, and interfaces, can affect the photovoltaic properties. The subsequently obtained VOC of 1.78 V is the highest recorded for single-junction PSCs to the best of our knowledge. Surprisingly, the conventional hole-transport layer spiro-OMeTAD, optimized for narrow bandgaps, sustains such high voltages. Photoluminescence measurements reveal a trap-assisted recombination peak at 1.65 eV, indicating deep traps as significant to voltage loss in MAPbCl3. KW - Perovskite solar cells KW - methylammonium lead trichloride (MAPbCl3) KW - uniform film crystallization KW - manipulation of annealing atmospheres KW - trap-assisted recombination KW - microstructure Y1 - 2024 U6 - https://doi.org/10.1021/acsenergylett.3c02777 SN - 2380-8195 VL - 9 SP - 1017 EP - 1024 ER - TY - GEN A1 - Kot, Małgorzata A1 - Kedia, Mayank A1 - Plate, Paul A1 - Marth, Ludwig A1 - Henkel, Karsten A1 - Flege, Jan Ingo T1 - Application of plasma enhanced atomic layer deposition process of alumina on perovskite film boosts efficiency of solar cells T2 - Verhandlungen der DPG N2 - It is assumed that plasma-enhanced atomic layer deposition (PEALD) cannot be used to prepare thin films on sensitive organic-inorganic perovskites because the plasma destroys the perovskite film and thus deteriorates its photophysical properties. Here, we prove that using an appropriate geometry of the ALD system (SENTECH SI PEALD system) and suitable process parameters it is possible to coat perovskites with alumina by PEALD. Spectromicroscopy followed by electrical characterisation reveal that as long as the PEALD process is not optimized (too long plasma pulses) one gets degradation of the perovskite as well as dissociation of the created iodine pentoxide (during PEALD) under light that causes a valence band maximum (VBM) shift to the Fermi level and thus significantly decreases the solar cell efficiency. However, once the PEALD process parameters are optimized, no VBM shift is observed. Moreover, the solar cell efficiency depends inversely on process temperature and layer thickness. KW - Plamsa-enhanced atomic layer deposition KW - Perovskite solar cells KW - Valence band maximum Y1 - 2023 UR - https://www.dpg-verhandlungen.de/year/2023/conference/skm/part/hl/session/4/contribution/2 SN - 0420-0195 PB - Deutsche Physikalische Gesellschaft CY - Bad Honnef ER - TY - GEN A1 - Kedia, Mayank A1 - Rai, Monika A1 - Phirke, Himanshu A1 - Aranda, Clara A. A1 - Das, Chittaranjan A1 - Chirvony, Vladimir A1 - Boehringer, Stephan A1 - Kot, Małgorzata A1 - Malekshahi Byranvand, Mahdi A1 - Flege, Jan Ingo A1 - Redinger, Alex A1 - Saliba, Michael T1 - Light Makes Right: Laser Polishing for Surface Modification of Perovskite Solar Cells T2 - ACS Energy Letters N2 - Interface engineering is a common strategy for passivating surface defects to attain open circuit voltages (Voc) in perovskite solar cells (PSCs). In this work, we introduce the concept of polishing a perovskite thin-film surface using a nanosecond (ns) pulsed ultraviolet laser to reduce surface defects, such as dangling bonds, undesirable phases, and suboptimal stoichiometry. A careful control of laser energy and scanning speed improves the photophysical properties of the surface without compromising the thickness. Using laser polishing, a Voc of 1.21 V is achieved for planar PSCs with a triple cation composition, showing an improved perovskite/hole transport interface by mitigating surface recombination losses. We measure an efficiency boost from 18.0% to 19.3% with improved stability of up to 1000 h. The results open the door to a new class of surface modification using lasers for interface passivation in well-controllable, automated, scalable, and solvent-free surface treatments. KW - Perovskite solar cells KW - laser polishing KW - perovskite/hole transport interface KW - surface defects KW - recombination losses Y1 - 2023 U6 - https://doi.org/10.1021/acsenergylett.3c00469 SN - 2380-8195 VL - 8 SP - 2603 EP - 2610 ER - TY - GEN A1 - Das, Chittaranjan A1 - Roy, Rajarshi A1 - Kedia, Mayank A1 - Kot, Małgorzata A1 - Zuo, Weiwei A1 - Félix, Roberto A1 - Sobol, Tomasz A1 - Flege, Jan Ingo A1 - Saliba, Michael T1 - Unraveling the Role of Perovskite in Buried Interface Passivation T2 - ACS Applied Materials & Interfaces N2 - Interfaces in perovskite solar cells play a crucial role in their overall performance, and therefore, detailed fundamental studies are needed for a better understanding. In the case of the classical n–i–p architecture, TiO2 is one of the most used electron-selective layers and can induce chemical reactions that influence the performance of the overall device stack. The interfacial properties at the TiO2/perovskite interface are often neglected, owing to the difficulty in accessing this interface. Here, we use X-rays of variable energies to study the interface of (compact and mesoporous) TiO2/perovskite in such a n–i–p architecture. The X-ray photoelectron spectroscopy and X-ray absorption spectroscopy methods show that the defect states present in the TiO2 layer are passivated by a chemical interaction of the perovskite precursor solution during the formation of the perovskite layer and form an organic layer at the interface. Such passivation of intrinsic defects in TiO2 removes charge recombination centers and shifts the bands upward. Therefore, interface defect passivation by oxidation of Ti3+ states, the organic cation layer, and an upward band bending at the TiO2/perovskite interface explain the origin of an improved electron extraction and hole-blocking nature of TiO2 in the n–i–p perovskite solar cells. KW - perovskite solar cells KW - interface KW - defects KW - photoemission spectroscopy Y1 - 2023 U6 - https://doi.org/10.1021/acsami.3c13085 SN - 1944-8244 SN - 1944-8252 VL - 15 IS - 48 SP - 56500 EP - 56510 ER - TY - GEN A1 - Kedia, Mayank A1 - Das, Chittaranjan A1 - Kot, Malgorzata A1 - Yalcinkaya, Yenal A1 - Zuo, Weiwei A1 - Tabah Tanko, Kenedy A1 - Matvija, Peter A1 - Ezquer, Mikel A1 - Cornago, Iñaki A1 - Hempel, Wolfram A1 - Kauffmann, Florian A1 - Plate, Paul A1 - Lira-Cantu, Monica A1 - Weber, Stefan A.L. A1 - Saliba, Michael T1 - Mitigating the amorphization of perovskite layers by using atomic layer deposition of alumina T2 - Energy & environmental science N2 - Atomic layer deposition of aluminum oxide (ALD-Al2O3) layers has recently been studied for stabilizing perovskite solar cells (PSCs) against environmental stressors, such as humidity and oxygen. In addition, the ALD-Al2O3 layer acts as a protective barrier, mitigating pernicious halide ion migration from the perovskite towards the hole transport interface. However, its effectiveness in preventing the infiltration of ions and additives from the hole-transport layer into perovskites remains insufficiently understood. Herein, we demonstrate the deposition of a compact ultrathin (∼0.75 nm) ALD-Al2O3 layer that conformally coats the morphology of a triple-cation perovskite layer. This promotes an effective contact of the hole transporter layer on top of the perovskite, thereby improving the charge carrier collection between these two layers. Upon systematically investigating the layer-by-layer structure of the PSC, we discovered that ALD-Al2O3 also acts as a diffusion barrier for the degraded species from the adjacent transport layer into the perovskite. In addition to these protective considerations, ALD-Al2O3 impedes the transition of crystalline perovskites to an undesired amorphous phase. Consequently, the dual functionality (i.e., enhanced contact and diffusion barrier) of the ALD-Al2O3 protection enhanced the device performance from 19.1% to 20.5%, while retaining 98% of its initial performance compared to <10% for pristine devices after 1500 h of outdoor testing under ambient conditions. Finally, this study deepens our understanding of the mechanism of ALD-Al2O3 as a two-way diffusion barrier, highlighting the multifaceted role of buffer layers in interfacial engineering for the long-term stability of PSCs. Y1 - 2025 U6 - https://doi.org/10.1039/D4EE05703A SN - 1754-5692 VL - 18 IS - 11 SP - 5250 EP - 5263 PB - Royal Society of Chemistry (RSC) CY - London ER -