TY - THES A1 - Canil, Laura T1 - Tuning Interfacial Properties in Perovskite Solar Cells through Defined Molecular Assemblies T1 - Anpassung von Grenzflächeneigenschaften von Perowskit-Solarzellen durch den Einsatz von molekularen Schichten N2 - In the frame of a world fighting a dramatic global warming caused by human-related activities, research towards the development of renewable energies plays a crucial role. Solar energy is one of the most important clean energy sources and its role in the satisfaction of the global energy demand is set to increase. In this context, a particular class of materials captured the attention of the scientific community for its attractive properties: halide perovskites. Devices with perovskite as light-absorber saw an impressive development within the last decade, reaching nowadays efficiencies comparable to mature photovoltaic technologies like silicon solar cells. Yet, there are still several roadblocks to overcome before a wide-spread commercialization of this kind of devices is enabled. One of the critical points lies at the interfaces: perovskite solar cells (PSCs) are made of several layers with different chemical and physical features. In order for the device to function properly, these properties have to be well-matched. This dissertation deals with some of the challenges related to interfaces in PSCs, with a focus on the interface between the perovskite material itself and the subsequent charge transport layer. In particular, molecular assemblies with specific properties are deposited on the perovskite surface to functionalize it. The functionalization results in energy level alignment adjustment, interfacial losses reduction, and stability improvement. First, a strategy to tune the perovskite’s energy levels is introduced: self-assembled monolayers of dipolar molecules are used to functionalize the surface, obtaining simultaneously a shift in the vacuum level position and a saturation of the dangling bonds at the surface. A shift in the vacuum level corresponds to an equal change in work function, ionization energy, and electron affinity. The direction of the shift depends on the direction of the collective interfacial dipole. The magnitude of the shift can be tailored by controlling the deposition parameters, such as the concentration of the solution used for the deposition. The shift for different molecules is characterized by several non-invasive techniques, including in particular Kelvin probe. Overall, it is shown that it is possible to shift the perovskite energy levels in both directions by several hundreds of meV. Moreover, interesting insights on the molecules deposition dynamics are revealed. Secondly, the application of this strategy in perovskite solar cells is explored. Devices with different perovskite compositions (“triple cation perovskite” and MAPbBr3) are prepared. The two resulting model systems present different energetic offsets at the perovskite/hole-transport layer interface. Upon tailored perovskite surface functionalization, the devices show a stabilized open circuit voltage (Voc) enhancement of approximately 60 meV on average for devices with MAPbBr3, while the impact is limited on triple-cation solar cells. This suggests that the proposed energy level tuning method is valid, but its effectiveness depends on factors such as the significance of the energetic offset compared to the other losses in the devices. Finally, the above presented method is further developed by incorporating the ability to interact with the perovskite surface directly into a novel hole-transport material (HTM), named PFI. The HTM can anchor to the perovskite halide ions via halogen bonding (XB). Its behaviour is compared to that of another HTM (PF) with same chemical structure and properties, except for the ability of forming XB. The interaction of perovskite with PFI and PF is characterized through UV-Vis, atomic force microscopy and Kelvin probe measurements combined with simulations. Compared to PF, PFI exhibits enhanced resilience against solvent exposure and improved energy level alignment with the perovskite layer. As a consequence, devices comprising PFI show enhanced Voc and operational stability during maximum-power-point tracking, in addition to hysteresis reduction. XB promotes the formation of a high-quality interface by anchoring to the halide ions and forming a stable and ordered interfacial layer, showing to be a particularly interesting candidate for the development of tailored charge transport materials in PSCs. Overall, the results exposed in this dissertation introduce and discuss a versatile tool to functionalize the perovskite surface and tune its energy levels. The application of this method in devices is explored and insights on its challenges and advantages are given. Within this frame, the results shed light on XB as ideal interaction for enhancing stability and efficiency in perovskite-based devices. N2 - Im Kampf gegen den menschengemachten Klimawandel spielt die Forschung und Entwicklung von erneuerbaren Energien eine tragende Rolle. Solarenergie ist eine der wichtigsten grünen Energiequellen und von steigender Bedeutung für die Deckung des globalen Energiebedarfs. In diesem Kontext hat eine bestimme Materialklasse aufgrund ihrer attraktiven Eigenschaften die Aufmerksamkeit der Wissenschaft erregt: Halogenid-Perowskit. Perowskit-Solarzellen haben im letzten Jahrzehnt eine beeindruckende Entwicklung durchgemacht und erreichen heutzutage Effizienzen, die mit weit entwickelten Photovoltaik-Technologien wie Silizium-Solarzellen vergleichbar sind. Jedoch existieren immer noch mehrere Hürden, die einer marktweiten Kommerzialisierung dieser jungen Technologie im Wege stehen. Eines der kritischen Probleme befindet sich an den Grenzflächen. Perowskit-Solarzellen bestehen aus mehreren Schichten mit unterschiedlichen chemischen und physikalischen Eigenschaften. Damit die Solarzelle bestmöglich funktioniert, müssen diese Eigenschaften aufeinander abgestimmt sein. Diese Dissertation beschäftigt sich mit einigen Herausforderungen im Zusammenhang mit Grenzflächen in Perowskit-Solarzellen, dabei liegt der Fokus auf der Grenzfläche zwischen Perowskit-Absorber und der angrenzenden Ladungstransportschicht. Insbesondere werden organische Moleküle mit spezifischen Eigenschaften verwendet um die Oberfläche des Perowskiten zu funktionalisieren. Dadurch wird eine Bandanpassung erreicht, Grenzflächenverluste reduziert und die Stabilität der Solarzellen erhöht. Zunächst wird eine Strategie zum Anpassen der Bandenergien vorgestellt: Selbst-organisierende Monoschichten dipolarer Moleküle werden auf die Perowskit-Oberfläche abgeschieden, um diese zu funktionalisieren. Dadurch wird eine Anpassung des Energie-Levels im Perowskiten und die Sättigung von ungebundenen Elektronenbindungen (engl. dangling bonds) an der Oberfläche erreicht. Die Richtung der Energielevel-Verschiebung hängt von der Richtung des kollektiven Grenzflächen-Dipols ab. Der Betrag der Energielevel-Verschiebung kann über die Depositionsparameter während der Schichtherstellung eingestellt werden. Die Energielevel-Verschiebung bei der Verwendung verschiedener Moleküle wird mit Hilfe verschiedener non-invasiver Charakterisierungsmethoden untersucht, insbesondere mit der Hilfe von Kelvin-Sonde Messungen. Diese Messungen ermöglichen interessante Erkenntnisse über die Dynamik der Deposition der Moleküle. Es ist möglich die Energielevel in beide Richtungen um mehrere hundert meV zu verschieben. Als Zweites wird die Anwendung dieser Stategie in Perowskit-Solarzellen erforscht. Solarzellen mit Perowskit-Absorbern unterschiedlicher Zusammensetzung (“Dreifach-Kationen-Perowskit” und MAPbBr3) werden präpariert; die beiden Modellsysteme besitzen dann unterschiedliche energetische Offsets an der Perowskit-Lochleiter Grenzfläche. Mit einer maßgeschneiderter Funktionalisierung der Perowskit-Oberfläche zeigen die MAPbBr3 Solarzellen eine permanente Verbesserung der offene-Klemmen-Spannung (engl. open circuit voltage, Voc) um durchschnittlich 60 meV, während der Einfluss auf die Solarzellen mit Dreifach-Kationen-Perowskit gering ist. Dies zeigt, dass die vorgestellte Methode zur Bandanpassung funktioniert, aber ihre Effektivität zudem von weiteren Faktoren abhängt: Die Relevanz des energetischen Offsets im Vergleich zu anderen Verlustmechanismen beeinflusst unter anderem die Effektivität der Funktionalisierung. Abschließend wird beschrieben, wie die präsentierte Methode zur Bandanpassung weiterentwickelt wird, indem das Vermögen, mit der Perowskit-Oberfläche zu interagieren, direkt in einen neuartigen Lochleiter („PFI“) integriert wird. Der Lochleiter kann sich über Halogenbindungen an den Perowskiten anlagern. Das Verhalten von PFI wird verglichen mit dem eines anderen Lochleiters („PF“), welcher die fast gleiche chemische Struktur und sehr ähnliche Eigenschaften aufweist, ausgenommen der Fähigkeit eine Halogenbindung zu formen. Die PFI-Perowskit und PF-Perowskit Interaktion wird durch UV-Vis Spektroskopie, Rasterkraftmikroskopie und Kelvin-Sonde Messungen, kombiniert mit Simulationen, charakterisiert. Beim direkten Vergleich von PFI und PF zeigt sich die Bildung der Halogenbindung in einer bei PFI verbesserten Widerstandskraft gegen Lösungsmittel und Bandanpassung zum Perowskiten. Beim Folgerichtig zeigen Solarzellen mit PFI zusätzlich zu einer verringerten Hysterese einen höheren Voc und eine erhöhte Stabilität während des Betriebs unter Maximum-Power-Point Tracking Zusammenfassend stellt diese Dissertation somit ein vielseitiges Werkzeug zur Funktionalisierung von Perowskit-Oberflächen und der dadurch erreichten Bandanpassung vor. Die Anwendung dieses Werkzeugs an Solarzellen wird erprobt und Einsichten in seine Vorteile und Nachteile erlangt. Die Halogenbindung wird als spezifische Interaktion identifiziert, die sich ideal zur Steigerung von Effizienz und Stabilität von Perowskit-basierten optoelektronischen Bauteilen erweisen könnte. KW - photovoltaic KW - perovskite solar cells KW - interfaces KW - energy levels KW - halogen bonding KW - Grenzflächen KW - Perowskit Solarzellen KW - Photovoltaik KW - Bandenenergien KW - Halogenbindung Y1 - 2021 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:kobv:517-opus4-546333 ER - TY - JOUR A1 - Zhang, Shanshan A1 - Hosseini, Seyed Mehrdad A1 - Gunder, Rene A1 - Petsiuk, Andrei A1 - Caprioglio, Pietro A1 - Wolff, Christian Michael A1 - Shoaee, Safa A1 - Meredith, Paul A1 - Schorr, Susan A1 - Unold, Thomas A1 - Burn, Paul L. A1 - Neher, Dieter A1 - Stolterfoht, Martin T1 - The Role of Bulk and Interface Recombination in High-Efficiency Low-Dimensional Perovskite Solar Cells JF - Advanced materials N2 - 2D Ruddlesden-Popper perovskite (RPP) solar cells have excellent environmental stability. However, the power conversion efficiency (PCE) of RPP cells remains inferior to 3D perovskite-based cells. Herein, 2D (CH3(CH2)(3)NH3)(2)(CH3NH3)(n-1)PbnI3n+1 perovskite cells with different numbers of [PbI6](4-) sheets (n = 2-4) are analyzed. Photoluminescence quantum yield (PLQY) measurements show that nonradiative open-circuit voltage (V-OC) losses outweigh radiative losses in materials with n > 2. The n = 3 and n = 4 films exhibit a higher PLQY than the standard 3D methylammonium lead iodide perovskite although this is accompanied by increased interfacial recombination at the top perovskite/C-60 interface. This tradeoff results in a similar PLQY in all devices, including the n = 2 system where the perovskite bulk dominates the recombination properties of the cell. In most cases the quasi-Fermi level splitting matches the device V-OC within 20 meV, which indicates minimal recombination losses at the metal contacts. The results show that poor charge transport rather than exciton dissociation is the primary reason for the reduction in fill factor of the RPP devices. Optimized n = 4 RPP solar cells had PCEs of 13% with significant potential for further improvements. KW - 2D perovskites KW - interface recombination KW - perovskite solar cells KW - photoluminescence KW - V-OC loss Y1 - 2019 U6 - https://doi.org/10.1002/adma.201901090 SN - 0935-9648 SN - 1521-4095 VL - 31 IS - 30 PB - Wiley-VCH CY - Weinheim ER - TY - THES A1 - Flatken, Marion A. T1 - The early stages of halide perovskites thin film formation T1 - Die frühen Stadien der Bildung von Halogenid-Perowskit-Dünnschichten N2 - As climate change worsens, there is a growing urgency to promote renewable energies and improve their accessibility to society. Here, solar energy harvesting is of particular importance. Currently, metal halide perovskite (MHP) solar cells are indispensable in future solar energy generation research. MHPs are crystalline semiconductors increasingly relevant as low-cost, high-performance materials for optoelectronics. Their processing from solution at low temperature enables easy fabrication of thin film elements, encompassing solar cells and light-emitting diodes or photodetectors. Understanding the coordination chemistry of MHPs in their precursor solution would allow control over the thin film crystallization, the material properties and the final device performance. In this work, we elaborate on the key parameters to manipulate the precursor solution with the long-term objective of enabling systematic process control. We focus on the nanostructural characterization of the initial arrangements of MHPs in the precursor solutions. Small-angle scattering is particularly well suited for measuring nanoparticles in solution. This technique proved to be valuable for the direct analyzes of perovskite precursor solutions in standard processing concentrations without causing radiation damage. We gain insights into the chemical nature of widely used precursor structures such as methylammonium lead iodide (MAPbI3), presenting first insights into the complex arrangements and interaction within this precursor state. Furthermore, we transfer the preceding results to other more complex perovskite precursors. The influence of compositional engineering is investigated using the addition of alkali cations as an example. As a result, we propose a detailed working mechanism on how the alkali cations suppress the formation of intermediate phases and improve the quality of the crystalline thin film. In addition, we investigate the crystallization process of a tin-based perovskite composition (FASnI3) under the influence of fluoride chemistry. We prove that the frequently used additive, tin fluoride (SnF2), selectively binds undesired oxidized tin (Sn(IV)) in the precursor solution. This prevents its incorporation into the actual crystal structure and thus reduces the defect density of the material. Furthermore, SnF2 leads to a more homogeneous crystal growth process, which results in improved crystal quality of the thin film material. In total, this study provides a detailed characterization of the complex system of perovskite precursor chemistry. We thereby cover relevant parameters for future MHP solar cell process control, such as (I) the environmental impact based on concentration and temperature (II) the addition of counter ions to reduce the diffuse layer surrounding the precursor nanostructures and (III) the targeted use of additives to eliminate unwanted components selectively and to ensure a more homogeneous crystal growth. N2 - Getrieben durch den Klimawandel wächst die Dringlichkeit erneuerbare Energien zu fördern und ihre Zugänglichkeit für die Gesellschaft zu verbessern. Solarenergie ist in dieser Hinsicht von besonderer Bedeutung. Derzeit sind Metallhalogenid-Perowskit-Solarzellen ein unverzichtbarer Bestandteil der Forschung an zukünftig klimaneutraler Energiegewinnung. Metallhalogenid-Perowskite (MHP) sind kristalline Halbleiter, die als kostengünstige und leistungsstarke Materialien für die Optoelektronik zunehmend an Bedeutung gewinnen. Ihre Verarbeitung aus Flüssigkeit bei niedriger Temperatur ermöglicht eine effiziente Herstellung von Dünnschichtelementen, zu denen nicht nur Solarzellen, sondern auch Leuchtdioden oder Photodetektoren zählen. Das Verständnis der Koordinationschemie in den Vorläuferlösungen der MHPs würde es daher ermöglichen, die Kristallisation der Dünnschichten, ihre Materialeigenschaften und die finale Leistung der entsprechenden Bauelemente zu kontrollieren. In dieser Arbeit werden die wichtigsten Parameter zur systematischen Beeinflussung der Vorläuferlösung ausgearbeitet, mit dem langfristigen Ziel eine systematische Prozesskontrolle zu ermöglichen. Dabei liegt ein Schwerpunkt auf der Anwendung einer nanostrukturellen Technik zur Charakterisierung erster Anordnungen in der Perowskit-Vorläuferlösung. Die Kleinwinkelstreuung eignet sich besonders gut zur nanostrukturellen Charakterisierung von entsprechenden Teilchen bzw. Clustern in Lösung. Mit dieser Methodik können wir auf direktem Wege Perowskit-Vorläuferlösungen in üblichen Verarbeitungs-konzentrationen analysieren. Wir erhalten Einblicke in die chemische Beschaffenheit der Vorläuferstrukturen und untersuchen zudem verschiedene Perowskit-Zusammensetzungen. Strukturelle Erkenntnisse über die Vorstufe im allgemein bekanntestem MHP, Methylammoniumbleijodid (MAPbI3) werden präsentiert und im Folgenden auf komplexere Anwendungen übertragen. Weiterhin wird der Einfluss von Kompositionsvariation am Beispiel der Zugabe von Alkali-Kationen (K, Rb, Cs) untersucht. Es wird ein detaillierter Wirkmechanismus vorgestellt, der erklärt, wie Alkali-Kationen die Bildung von Zwischenphasen unterdrücken und zudem die Qualität der kristallinen Dünnschicht verbessern. Unter Berücksichtigung vorangehender Ergebnisse, thematisiert diese Arbeit zudem den Kristallisationsprozess einer zinnbasierten Perowskit-Zusammensetzung (FASnI3) unter dem Einfluss von Fluoridchemie. Das häufig zugesetzte Additiv, Zinnfluorid (SnF2), bindet selektiv unerwünschtes, oxidiertes Sn(IV) bereits in der Vorläuferlösung. Dieses verhindert dessen Einbau in die eigentliche Kristallstruktur und verringert so die Defektdichte des Materials. Darüber hinaus führt SnF2 zu einem homogeneren Kristallwachstumsprozess, was eine bessere Kristallqualität des Dünnschichtmaterials und somit final eine bessere Solarzellenleistung zur Folge hat. Insgesamt bietet diese Studie eine detaillierte Charakterisierung des komplexen Systems der Perowskit-Vorläuferchemie und liefert dabei notwendige Parameter, die für die zukünftige Prozesssteuerung von Relevanz sind. KW - perovskite solar cells KW - perovskite precursors KW - thin film crystallization KW - small-angle scattering KW - Perowskit Solarzellen KW - Perowskit Vorläuferstadien KW - Kristallisation von Dünnschichten KW - Kleinwinkelstreuung Y1 - 2022 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:kobv:517-opus4-552599 ER - TY - THES A1 - Hussein, Mahmoud T1 - Solvent engineering for highly-efficiency lead-free perovskite solar cells T1 - Lösungsmitteltechnik für hocheffiziente Zinn-Perowskit-Solarzellen N2 - Global warming, driven primarily by the excessive emission of greenhouse gases such as carbon dioxide into the atmosphere, has led to severe and detrimental environmental impacts. Rising global temperatures have triggered a cascade of adverse effects, including melting glaciers and polar ice caps, more frequent and intense heat waves disrupted weather patterns, and the acidification of oceans. These changes adversely affect ecosystems, biodiversity, and human societies, threatening food security, water availability, and livelihoods. One promising solution to mitigate the harmful effects of global warming is the widespread adoption of solar cells, also known as photovoltaic cells. Solar cells harness sunlight to generate electricity without emitting greenhouse gases or other pollutants. By replacing fossil fuel-based energy sources, solar cells can significantly reduce CO2 emissions, a significant contributor to global warming. This transition to clean, renewable energy can help curb the increasing concentration of greenhouse gases in the atmosphere, thereby slowing down the rate of global temperature rise. Solar energy’s positive impact extends beyond emission reduction. As solar panels become more efficient and affordable, they empower individuals, communities, and even entire nations to generate electricity and become less dependent on fossil fuels. This decentralized energy generation can enhance resilience in the face of climate-related challenges. Moreover, implementing solar cells creates green jobs and stimulates technological innovation, further promoting sustainable economic growth. As solar technology advances, its integration with energy storage systems and smart grids can ensure a stable and reliable energy supply, reducing the need for backup fossil fuel power plants that exacerbate environmental degradation. The market-dominant solar cell technology is silicon-based, highly matured technology with a highly systematic production procedure. However, it suffers from several drawbacks, such as: 1) Cost: still relatively high due to high energy consumption due to the need to melt and purify silicon, and the use of silver as an electrode, which hinders their widespread availability, especially in low-income countries. 2) Efficiency: theoretically, it should deliver around 29%; however, the efficiency of most of the commercially available silicon-based solar cells ranges from 18 – 22%. 3) Temperature sensitivity: The efficiency decreases with the increase in the temperature, affecting their output. 4) Resource constraints: silicon as a raw material is unavailable in all countries, creating supply chain challenges. Perovskite solar cells arose in 2011 and matured very rapidly in the last decade as a highly efficient and versatile solar cell technology. With an efficiency of 26%, high absorption coefficients, solution processability, and tunable band gap, it attracted the attention of the solar cells community. It represented a hope for cheap, efficient, and easily processable next-generation solar cells. However, lead toxicity might be the block stone hindering perovskite solar cells’ market reach. Lead is a heavy and bioavailable element that makes perovskite solar cells environmentally unfriendly technology. As a result, scientists try to replace lead with a more environmentally friendly element. Among several possible alternatives, tin was the most suitable element due to its electronic and atomic structure similarity to lead. Tin perovskites were developed to alleviate the challenge of lead toxicity. Theoretically, it shows very high absorption coefficients, an optimum band gap of 1.35 eV for FASnI3, and a very high short circuit current, which nominates it to deliver the highest possible efficiency of a single junction solar cell, which is around 30.1% according to Schockly-Quisser limit. However, tin perovskites’ efficiency still lags below 15% and is irreproducible, especially from lab to lab. This humble performance could be attributed to three reasons: 1) Tin (II) oxidation to tin (IV), which would happen due to oxygen, water, or even by the effect of the solvent, as was discovered recently. 2) fast crystallization dynamics, which occurs due to the lateral exposure of the P-orbitals of the tin atom, which enhances its reactivity and increases the crystallization pace. 3) Energy band misalignment: The energy bands at the interfaces between the perovskite absorber material and the charge selective layers are not aligned, leading to high interfacial charge recombination, which devastates the photovoltaic performance. To solve these issues, we implemented several techniques and approaches that enhanced the efficiency of tin halide perovskites, providing new chemically safe solvents and antisolvents. In addition, we studied the energy band alignment between the charge transport layers and the tin perovskite absorber. Recent research has shown that the principal source of tin oxidation is the solvent known as dimethylsulfoxide, which also happens to be one of the most effective solvents for processing perovskite. The search for a stable solvent might prove to be the factor that makes all the difference in the stability of tin-based perovskites. We started with a database of over 2,000 solvents and narrowed it down to a series of 12 new solvents that are suitable for processing FASnI3 experimentally. This was accomplished by looking into 1) the solubility of the precursor chemicals FAI and SnI2, 2) the thermal stability of the precursor solution, and 3) the potential to form perovskite. Finally, we show that it is possible to manufacture solar cells using a novel solvent system that outperforms those produced using DMSO. The results of our research give some suggestions that may be used in the search for novel solvents or mixes of solvents that can be used to manufacture stable tin-based perovskites. Due to the quick crystallization of tin, it is more difficult to deposit tin-based perovskite films from a solution than manufacturing lead-based perovskite films since lead perovskite is more often utilized. The most efficient way to get high efficiencies is to deposit perovskite from dimethyl sulfoxide (DMSO), which slows down the quick construction of the tin-iodine network that is responsible for perovskite synthesis. This is the most successful approach for achieving high efficiencies. Dimethyl sulfoxide, which is used in the processing, is responsible for the oxidation of tin, which is a disadvantage of this method. This research presents a potentially fruitful alternative in which 4-(tert-butyl) pyridine can substitute dimethyl sulfoxide in the process of regulating crystallization without causing tin oxidation to take place. Perovskite films that have been formed from pyridine have been shown to have a much-reduced defect density. This has resulted in increased charge mobility and better photovoltaic performance, making pyridine a desirable alternative for use in the deposition of tin perovskite films. The precise control of perovskite precursor crystallization inside a thin film is of utmost importance for optimizing the efficiency and manufacturing of solar cells. The deposition process of tin-based perovskite films from a solution presents difficulties due to the quick crystallization of tin compared to the more often employed lead perovskite. The optimal approach for attaining elevated efficiencies entails using dimethyl sulfoxide (DMSO) as a medium for depositing perovskite. This choice of solvent impedes the tin-iodine network’s fast aggregation, which plays a crucial role in the production of perovskite. Nevertheless, this methodology is limited since the utilization of dimethyl sulfoxide leads to the oxidation of tin throughout the processing stage. In this thesis, we present a potentially advantageous alternative approach wherein 4-(tert-butyl) pyridine is proposed as a substitute for dimethyl sulfoxide in regulating crystallization processes while avoiding the undesired consequence of tin oxidation. Films of perovskite formed using pyridine as a solvent have a notably reduced density of defects, resulting in higher mobility of charges and improved performance in solar applications. Consequently, the utilization of pyridine for the deposition of tin perovskite films is considered advantageous. Tin perovskites are suffering from an apparent energy band misalignment. However, the band diagrams published in the current body of research display contradictions, resulting in a dearth of unanimity. Moreover, comprehensive information about the dynamics connected with charge extraction is lacking. This thesis aims to ascertain the energy band locations of tin perovskites by employing the kelvin probe and Photoelectron yield spectroscopy methods. This thesis aims to construct a precise band diagram for the often-utilized device stack. Moreover, a comprehensive analysis is performed to assess the energy deficits inherent in the current energetic structure of tin halide perovskites. In addition, we investigate the influence of BCP on the improvement of electron extraction in C60/BCP systems, with a specific emphasis on the energy factors involved. Furthermore, transient surface photovoltage was utilized to investigate the charge extraction kinetics of frequently studied charge transport layers, such as NiOx and PEDOT as hole transport layers and C60, ICBA, and PCBM as electron transport layers. The Hall effect, KP, and TRPL approaches accurately ascertain the p-doping concentration in FASnI3. The results consistently demonstrated a value of 1.5 * 1017 cm-3. Our research findings highlight the imperative nature of autonomously constructing the charge extraction layers for tin halide perovskites, apart from those used for lead perovskites. The crystallization of perovskite precursors relies mainly on the utilization of two solvents. The first one dissolves the perovskite powder to form the precursor solution, usually called the solvent. The second one precipitates the perovskite precursor, forming the wet film, which is a supersaturated solution of perovskite precursor and in the remains of the solvent and the antisolvent. Later, this wet film crystallizes upon annealing into a full perovskite crystallized film. In our research context, we proposed new solvents to dissolve FASnI3, but when we tried to form a film, most of them did not crystallize. This is attributed to the high coordination strength between the metal halide and the solvent molecules, which is unbreakable by the traditionally used antisolvents such as Toluene and Chlorobenzene. To solve this issue, we introduce a high-throughput antisolvent screening in which we screened around 73 selected antisolvents against 15 solvents that can form a 1M FASnI3 solution. We used for the first time in tin perovskites machine learning algorithm to understand and predict the effect of an antisolvent on the crystallization of a precursor solution in a particular solvent. We relied on film darkness as a primary criterion to judge the efficacy of a solvent-antisolvent pair. We found that the relative polarity between solvent and antisolvent is the primary factor that affects the solvent-antisolvent interaction. Based on our findings, we prepared several high-quality tin perovskite films free from DMSO and achieved an efficiency of 9%, which is the highest DMSO tin perovskite device so far. N2 - Zinn ist eine der vielversprechendsten Alternativen zu Blei, um bleifreie Halogenidperowskite für die Optoelektronik herzustellen. Die Stabilität von Perowskiten auf Zinnbasis wird jedoch durch die Oxidation von Sn(II) zu Sn(IV) beeinträchtigt. Jüngste Arbeiten haben ergeben, dass Dimethylsulfoxid, eines der besten Lösungsmittel für die Verarbeitung von Perowskiten, die Hauptquelle für die Oxidation von Zinn ist. Die Suche nach einem stabilen Lösungsmittel könnte den Ausschlag für die Stabilität von Perowskiten auf Zinnbasis geben. Ausgehend von einer Datenbank mit über 2000 Lösungsmitteln haben wir eine Reihe von 12 neuen Lösungsmitteln identifiziert, die für die Verarbeitung von Formamidinium-Zinniodid-Perowskit (FASnI3) geeignet sind, indem wir 1) die Löslichkeit der Vorläuferchemikalien FAI und SnI2, 2) die thermische Stabilität der Vorläuferlösung und 3) die Möglichkeit zur Bildung von Perowskit experimentell untersucht haben. Schließlich demonstrieren wir ein neues Lösungsmittelsystem zur Herstellung von Solarzellen, das die auf DMSO basierenden Zellen übertrifft. Unsere Arbeit liefert Leitlinien für die weitere Identifizierung neuer Lösungsmittel oder Lösungsmittelmischungen zur Herstellung stabiler Perowskite auf Zinnbasis. Die genaue Steuerung der Kristallisation des Perowskit-Vorläufers in einer Dünnschicht ist entscheidend für die Effizienz und Produktion von Solarzellen. Die Abscheidung von Perowskit-Filmen auf Zinnbasis aus einer Lösung stellt aufgrund der schnellen Kristallisation von Zinn im Vergleich zu dem üblicherweise verwendeten Bleiperowskit eine Herausforderung dar. Die effektivste Methode zur Erzielung hoher Wirkungsgrade ist die Abscheidung von Perowskit aus Dimethylsulfoxid (DMSO), das den schnellen Aufbau des für die Perowskitbildung verantwortlichen Zinn-Jod-Netzwerks behindert. Dieser Ansatz hat jedoch einen Nachteil, da Dimethylsulfoxid während der Verarbeitung eine Zinnoxidation verursacht. In dieser Studie wird eine vielversprechende Alternative vorgestellt, bei der 4-(tert-Butyl)-pyridin Dimethylsulfoxid bei der Steuerung der Kristallisation ersetzen kann, ohne eine Zinnoxidation zu verursachen. Aus Pyridin abgeschiedene Perowskit-Filme weisen eine deutlich geringere Defektdichte auf, was zu einer erhöhten Ladungsbeweglichkeit und einer verbesserten photovoltaischen Leistung führt und es zu einer günstigen Wahl für die Abscheidung von Zinn-Perowskit-Filmen macht. Zinnperowskite haben sich als vielversprechender, umweltverträglicher Ersatz für Bleiperowskite erwiesen, vor allem wegen ihrer besseren optoelektronischen Eigenschaften und ihrer geringeren Bioverfügbarkeit. Dennoch gibt es mehrere Gründe, warum die Leistung von Zinnperowskiten nicht mit der von Bleiperowskiten verglichen werden kann. Einer dieser Gründe ist die Nichtübereinstimmung der Energiebänder zwischen dem Perowskit-Absorberfilm und den ladungstransportierenden Schichten (CTLs). Die in der vorhandenen Literatur dargestellten Banddiagramme sind jedoch uneinheitlich, was zu einem Mangel an Konsens führt. Außerdem ist das Verständnis der mit der Ladungsextraktion verbundenen Dynamik noch unzureichend. In dieser Studie sollen die Energiebandpositionen von Zinnperowskiten mit Hilfe der Kelvinsonde (KP) und der Photoelektronenausbeutespektroskopie (PYS) bestimmt werden. Ziel ist es, ein genaues Banddiagramm für den üblicherweise verwendeten Bauelementestapel zu erstellen. Darüber hinaus führen wir eine Diagnose der energetischen Unzulänglichkeiten durch, die im bestehenden energetischen Rahmen von Zinnhalogenid-Perowskiten vorhanden sind. Unser Ziel ist es, Folgendes zu klären den Einfluss von BCP auf die Verbesserung der Elektronenextraktion in C60/BCP-Systemen, wobei der Schwerpunkt auf den energetischen Aspekten liegt. Darüber hinaus haben wir die transiente Oberflächenphotospannung (tr-SPV) eingesetzt, um Einblicke in die Ladungsextraktionskinetik von allgemein bekannten CTLs zu gewinnen, einschließlich NiOx und PEDOT als Lochtransportschichten (HTLs) und C60, ICBA und PCBM als Elektronentransportschichten (ETLs). In diesem Kapitel verwenden wir den Halleffekt, KP- und TRPL-Techniken, um die genaue p-Dotierungskonzentration in FASnI3 zu bestimmen. Unsere Ergebnisse ergaben durchweg einen Wert von 1.5 * 1017 cm-3. Die Ergebnisse unserer Studie zeigen, dass es notwendig ist, die Ladungsextraktionsschichten von Zinnhalogenidperowskiten unabhängig von den Bleiperowskiten zu entwickeln. Die Kristallisation von Perowskit-Vorstufen beruht hauptsächlich auf der Verwendung von zwei Lösungsmitteln. Das erste löst das Perowskit-Pulver auf und bildet die Vorläuferlösung, die üblicherweise als Lösungsmittel bezeichnet wird. Mit dem zweiten wird der Perowskit-Precursor ausgefällt, wobei sich der Nassfilm bildet, der eine übersättigte Lösung des Perowskit-Precursors und der Reste des Lösungsmittels und des Antisolierungsmittels ist. Später kristallisiert dieser nasse Film beim Ausglühen zu einem vollständig kristallisierten Perowskit-Film. In unserem Forschungskontext haben wir neue Lösungsmittel vorgeschlagen, um FASnI3 aufzulösen, aber als wir versuchten, einen Film zu bilden, kristallisierten die meisten von ihnen nicht. Dies ist auf die hohe Koordinationsstärke zwischen dem Metallhalogenid und den Lösungsmittelmolekülen zurückzuführen, die von den traditionell verwendeten Antisolierungsmitteln wie Toluol und Chlorbenzol nicht aufgebrochen werden kann. Um dieses Problem zu lösen, haben wir ein Hochdurchsatz-Screening von Antisolventien durchgeführt, bei dem wir 73 ausgewählte Antisolventien mit 15 Lösungsmitteln verglichen haben, die eine 1M FASnI3-Lösung bilden können. Wir haben zum ersten Mal bei Zinnperowskiten einen Algorithmus für maschinelles Lernen verwendet, um die Wirkung eines Antisolvens auf die Kristallisation einer Vorläuferlösung in einem bestimmten Lösungsmittel zu verstehen und vorherzusagen. Wir stützten uns auf die Schwärzung des Films als primäres Kriterium zur Beurteilung der Wirksamkeit eines Lösungsmittel-Antisolierungsmittel-Paares. Wir fanden heraus, dass die relative Polarität zwischen Lösungsmittel und Antisolvent der wichtigste Faktor ist, der die Wechselwirkung zwischen Lösungsmittel und Antisolvent beeinflusst. Auf der Grundlage unserer Erkenntnisse haben wir mehrere hochwertige Zinn-Perowskit-Filme ohne DMSO hergestellt und einen Wirkungsgrad von 9 % erzielt, was die bisher höchste DMSO-Zinn-Perowskit-Vorrichtung darstellt. KW - perovskite solar cells KW - lead-free perovskites KW - tin perovskites KW - solar cells KW - perovskite KW - Perowskit-Solarzellen KW - photovoltaische Materialien KW - Solarzellen KW - Lösungsmittel KW - bleifreie Perowskit-Solarzellen Y1 - 2024 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:kobv:517-opus4-630375 ER - TY - JOUR A1 - Wolff, Christian Michael A1 - Zu, Fengshuo A1 - Paulke, Andreas A1 - Toro, Lorena Perdigon A1 - Koch, Norbert A1 - Neher, Dieter T1 - Reduced Interface-Mediated Recombination for High Open-Circuit Voltages in CH3NH3PbI3 Solar Cells JF - Advanced materials N2 - Perovskite solar cells with all-organic transport layers exhibit efficiencies rivaling their counterparts that employ inorganic transport layers, while avoiding high-temperature processing. Herein, it is investigated how the choice of the fullerene derivative employed in the electron-transporting layer of inverted perovskite cells affects the open-circuit voltage (V-OC). It is shown that nonradiative recombination mediated by the electron-transporting layer is the limiting factor for the V-OC in the cells. By inserting an ultrathin layer of an insulating polymer between the active CH3NH3PbI3 perovskite and the fullerene, an external radiative efficiency of up to 0.3%, a V-OC as high as 1.16 V, and a power conversion efficiency of 19.4% are realized. The results show that the reduction of nonradiative recombination due to charge-blocking at the perovskite/organic interface is more important than proper level alignment in the search for ideal selective contacts toward high V-OC and efficiency. KW - electron-transport layers KW - nonradiative recombination KW - open-circuit voltage KW - perovskite solar cells Y1 - 2017 U6 - https://doi.org/10.1002/adma.201700159 SN - 0935-9648 SN - 1521-4095 VL - 29 PB - Wiley-VCH CY - Weinheim ER - TY - JOUR A1 - Wang, Qiong A1 - Mosconi, Edoardo A1 - Wolff, Christian Michael A1 - Li, Junming A1 - Neher, Dieter A1 - De Angelis, Filippo A1 - Suranna, Gian Paolo A1 - Grisorio, Roberto A1 - Abate, Antonio T1 - Rationalizing the molecular design of hole-selective contacts to improve charge extraction in Perovskite solar cells JF - dvanced energy materials N2 - Two new hole selective materials (HSMs) based on dangling methylsulfanyl groups connected to the C-9 position of the fluorene core are synthesized and applied in perovskite solar cells. Being structurally similar to a half of Spiro-OMeTAD molecule, these HSMs (referred as FS and DFS) share similar redox potentials but are endowed with slightly higher hole mobility, due to the planarity and large extension of their structure. Competitive power conversion efficiency (up to 18.6%) is achieved by using the new HSMs in suitable perovskite solar cells. Time-resolved photoluminescence decay measurements and electrochemical impedance spectroscopy show more efficient charge extraction at the HSM/perovskite interface with respect to Spiro-OMeTAD, which is reflected in higher photocurrents exhibited by DFS/FS-integrated perovskite solar cells. Density functional theory simulations reveal that the interactions of methylammonium with methylsulfanyl groups in DFS/FS strengthen their electrostatic attraction with the perovskite surface, providing an additional path for hole extraction compared to the sole presence of methoxy groups in Spiro-OMeTAD. Importantly, the low-cost synthesis of FS makes it significantly attractive for the future commercialization of perovskite solar cells. KW - hole extraction KW - hole selective materials KW - perovskite solar cells KW - sulfur KW - triple-cation perovskite Y1 - 2019 U6 - https://doi.org/10.1002/aenm.201900990 SN - 1614-6832 SN - 1614-6840 VL - 9 IS - 28 PB - Wiley-VCH CY - Weinheim ER - TY - JOUR A1 - Le Corre, Vincent M. A1 - Diekmann, Jonas A1 - Peña-Camargo, Francisco A1 - Thiesbrummel, Jarla A1 - Tokmoldin, Nurlan A1 - Gutierrez-Partida, Emilio A1 - Peters, Karol Pawel A1 - Perdigón-Toro, Lorena A1 - Futscher, Moritz H. A1 - Lang, Felix A1 - Warby, Jonathan A1 - Snaith, Henry J. A1 - Neher, Dieter A1 - Stolterfoht, Martin T1 - Quantification of efficiency losses due to mobile ions in Perovskite solar cells via fast hysteresis measurements JF - Solar RRL N2 - Perovskite semiconductors differ from most inorganic and organic semiconductors due to the presence of mobile ions in the material. Although the phenomenon is intensively investigated, important questions such as the exact impact of the mobile ions on the steady-state power conversion efficiency (PCE) and stability remain. Herein, a simple method is proposed to estimate the efficiency loss due to mobile ions via "fast-hysteresis" measurements by preventing the perturbation of mobile ions out of their equilibrium position at fast scan speeds (approximate to 1000 V s(-1)). The "ion-free" PCE is between 1% and 3% higher than the steady-state PCE, demonstrating the importance of ion-induced losses, even in cells with low levels of hysteresis at typical scan speeds (approximate to 100mv s(-1)). The hysteresis over many orders of magnitude in scan speed provides important information on the effective ion diffusion constant from the peak hysteresis position. The fast-hysteresis measurements are corroborated by transient charge extraction and capacitance measurements and numerical simulations, which confirm the experimental findings and provide important insights into the charge carrier dynamics. The proposed method to quantify PCE losses due to field screening induced by mobile ions clarifies several important experimental observations and opens up a large range of future experiments. KW - hysteresis KW - mobile ions KW - perovskite solar cells Y1 - 2021 U6 - https://doi.org/10.1002/solr.202100772 SN - 2367-198X VL - 6 IS - 4 PB - Wiley-VCH CY - Weinheim ER - TY - GEN A1 - Caprioglio, Pietro A1 - Stolterfoht, Martin A1 - Wolff, Christian Michael A1 - Unold, Thomas A1 - Rech, Bernd A1 - Albrecht, Steve A1 - Neher, Dieter T1 - On the relation between the open‐circuit voltage and quasi‐Fermi level splitting in efficient perovskite solar cells T2 - Postprints der Universität Potsdam Mathematisch-Naturwissenschaftliche Reihe N2 - Today's perovskite solar cells (PSCs) are limited mainly by their open‐circuit voltage (VOC) due to nonradiative recombination. Therefore, a comprehensive understanding of the relevant recombination pathways is needed. Here, intensity‐dependent measurements of the quasi‐Fermi level splitting (QFLS) and of the VOC on the very same devices, including pin‐type PSCs with efficiencies above 20%, are performed. It is found that the QFLS in the perovskite lies significantly below its radiative limit for all intensities but also that the VOC is generally lower than the QFLS, violating one main assumption of the Shockley‐Queisser theory. This has far‐reaching implications for the applicability of some well‐established techniques, which use the VOC as a measure of the carrier densities in the absorber. By performing drift‐diffusion simulations, the intensity dependence of the QFLS, the QFLS‐VOC offset and the ideality factor are consistently explained by trap‐assisted recombination and energetic misalignment at the interfaces. Additionally, it is found that the saturation of the VOC at high intensities is caused by insufficient contact selectivity while heating effects are of minor importance. It is concluded that the analysis of the VOC does not provide reliable conclusions of the recombination pathways and that the knowledge of the QFLS‐VOC relation is of great importance. T3 - Zweitveröffentlichungen der Universität Potsdam : Mathematisch-Naturwissenschaftliche Reihe - 774 KW - electro‐optical materials KW - perovskite solar cells KW - photovoltaic devices KW - thin films Y1 - 2019 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:kobv:517-opus4-437595 SN - 1866-8372 IS - 774 ER - TY - JOUR A1 - Caprioglio, Pietro A1 - Stolterfoht, Martin A1 - Wolff, Christian Michael A1 - Unold, Thomas A1 - Rech, Bernd A1 - Albrecht, Steve A1 - Neher, Dieter T1 - On the relation between the open-circuit voltage and quasi-fermi level splitting in efficient perovskite solar cells JF - advanced energy materials N2 - Today's perovskite solar cells (PSCs) are limited mainly by their open‐circuit voltage (VOC) due to nonradiative recombination. Therefore, a comprehensive understanding of the relevant recombination pathways is needed. Here, intensity‐dependent measurements of the quasi‐Fermi level splitting (QFLS) and of the VOC on the very same devices, including pin‐type PSCs with efficiencies above 20%, are performed. It is found that the QFLS in the perovskite lies significantly below its radiative limit for all intensities but also that the VOC is generally lower than the QFLS, violating one main assumption of the Shockley‐Queisser theory. This has far‐reaching implications for the applicability of some well‐established techniques, which use the VOC as a measure of the carrier densities in the absorber. By performing drift‐diffusion simulations, the intensity dependence of the QFLS, the QFLS‐VOC offset and the ideality factor are consistently explained by trap‐assisted recombination and energetic misalignment at the interfaces. Additionally, it is found that the saturation of the VOC at high intensities is caused by insufficient contact selectivity while heating effects are of minor importance. It is concluded that the analysis of the VOC does not provide reliable conclusions of the recombination pathways and that the knowledge of the QFLS‐VOC relation is of great importance. KW - electro-optical materials KW - perovskite solar cells KW - photovoltaic devices KW - thin films Y1 - 2019 U6 - https://doi.org/10.1002/aenm.201901631 SN - 1614-6832 SN - 1614-6840 VL - 9 IS - 33 PB - Wiley-VCH CY - Weinheim ER - TY - JOUR A1 - Sandberg, Oskar J. A1 - Kurpiers, Jona A1 - Stolterfoht, Martin A1 - Neher, Dieter A1 - Meredith, Paul A1 - Shoaee, Safa A1 - Armin, Ardalan T1 - On the question of the need for a built-in potential in Perovskite solar cells JF - Advanced materials interfaces N2 - Perovskite semiconductors as the active materials in efficient solar cells exhibit free carrier diffusion lengths on the order of microns at low illumination fluxes and many hundreds of nanometers under 1 sun conditions. These lengthscales are significantly larger than typical junction thicknesses, and thus the carrier transport and charge collection should be expected to be diffusion controlled. A consensus along these lines is emerging in the field. However, the question as to whether the built-in potential plays any role is still of matter of some conjecture. This important question using phase-sensitive photocurrent measurements and theoretical device simulations based upon the drift-diffusion framework is addressed. In particular, the role of the built-in electric field and charge-selective transport layers in state-of-the-art p-i-n perovskite solar cells comparing experimental findings and simulation predictions is probed. It is found that while charge collection in the junction does not require a drift field per se, a built-in potential is still needed to avoid the formation of reverse electric fields inside the active layer, and to ensure efficient extraction through the charge transport layers. KW - built-in potential KW - charge collection KW - charge transport layers KW - perovskite solar cells Y1 - 2020 U6 - https://doi.org/10.1002/admi.202000041 SN - 2196-7350 VL - 7 IS - 10 PB - Wiley CY - Hoboken ER -