Most efficient perovskite solar cells are based on polycrystalline thin films; however, substantial structural disorder and defective grain boundaries place a limit on their performance. Perovskite single crystals are free of grain boundaries, leading to significantly low defect densities and thus hold promise for high-efficiency photovoltaics. However, the surfaces of perovskite single crystals present a major performance bottleneck because they possess a higher density of traps than the bulk. Hence, it is crucial to understand and control the surface trap population to fully exploit perovskite single crystals. This perspective highlights the importance of surface-trap management in unleashing the potential of perovskite single-crystal photovoltaics and discusses strategies to take this technology beyond the proof-of-concept stage.
Despite
the well-known implications in the field of III–V
semiconductors, lattice strain in halide perovskite materials has
been largely overlooked until recently. Here, we review the effect
of lattice strain on the structural, chemical, and optoelectronic
properties of metal halide perovskites to understand how strain engineering
can be applied to improve device performance. We start by arguing
that perovskites, like any other semiconducting material, are not
immune to the negative effects of mismanaged strain. We analyze the
originand detrimental consequencesof lattice strain
in perovskite crystals and heterostructures. We then discuss how strain
management addresses the polymorphism issue of some of the most desirable
perovskite compositions, and how it prevents the harmful migration
of ions in perovskites. We conclude by offering our perspective on
the unexplored potential of strain engineering and argue that its
controlled management can lead to untapped territories, including
perovskite large-area single-crystalline thin films and electrically
pumped lasers.
Lead (Pb) in conventional perovskite solar cells (PSCs) is toxic and has to be replaced. Situated in one group of the periodic table of elements, tin (Sn) has the same valence electrons' configuration as Pb (ns 2 np 2 ), promising analogous chemical properties. Hence, Sn is considered a suitable replacement to Pb. However, because of the lack of lanthanide shrinkage, Sn behaves differently: Pb is stable in Pb 2+ form, an oxidation state needed for perovskite structure, while Sn tends to lose all its valence electrons forming Sn 4+ . As a result, PSCs based on Sn are not efficient. Traces of oxygen have been conventionally discussed as a source of Sn oxidation. But recent findings point to the oxidation of Sn-based perovskites even in the absence of oxygen. This perspective summarizes recentlydiscovered unconventional oxidation pathways of Sn perovskites, including reaction with solvent molecules and disproportionation. We explain these phenomena by a Frost−Ebsworth diagram and argue that a deeper understanding of this diagram is a key toward stable and efficient Pb-free Sn-based PSCs.
Lead-free
halide light-emitting diodes (LEDs) are fabricated using
nontoxic and earth-abundant CsCu2I3 with a strong
yellow emission at a peak wavelength of 568 nm. CsCu2I3-based host–dopant emitters are formed by vacuum thermal
evaporation (VTE) film codeposition process instead of the commonly
used solution-based film deposition process. Using the VTE process,
extremely thin (30 nm) host–dopant emitters have successfully
been formed with the CsCu2I3 dopant and various
organic host molecules. A bright yellow emission with a photoluminescence
quantum yield value of 84.8% is achieved in the 0.5% CsCu2I3-doped halide emitter film due to the successful spatial
localization of charge carriers and excitons using an organic host
with appropriate energy levels to CsCu2I3. With
the further enhancement in charge balance using the cohost system,
a record-breaking lead-free halide LED has been fabricated with an
EQE of 7.4%. The lead-free halide LEDs are also highly stable in the
device operation with LT70 of 20 h at 100 cd/m2.
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