19 research outputs found
In Operando, Photovoltaic, and Microscopic Evaluation of Recombination Centers in Halide Perovskite-Based Solar Cells
The origin of the low densities of electrically active defects in Pb halide perovskite (HaP), a crucial factor for their use in photovoltaics, light emission, and radiation detection, remains a matter of discussion, in part because of the difficulty in determining these densities. Here, we present a powerful approach to assess the defect densities, based on electric field mapping in working HaP-based solar cells. The minority carrier diffusion lengths were deduced from the electric field profile, measured by electron beam-induced current (EBIC). The EBIC method was used earlier to get the first direct evidence for the n-i-p junction structure, at the heart of efficient HaP-based PV cells, and later by us and others for further HaP studies. This manuscript includes EBIC results on illuminated cell cross sections (in operando) at several light intensities to compare optoelectronic characteristics of different cells made by different groups in several laboratories. We then apply a simple, effective single-level defect model that allows deriving the densities (Nr) of the defect acting as recombination center. We find Nr â 1 Ă 1013 cmâ3 for mixed A cation lead bromide-based HaP films and âŒ1 Ă 1014 cmâ3 for MAPbBr3(Cl). As EBIC photocurrents are similar at the grain bulk and boundaries, we suggest that the defects are at the interfaces with selective contacts rather than in the HaP film. These results are relevant for photovoltaic devices as the EBIC responses distinguish clearly between high- and low-efficiency devices. The most efficient devices have n-i-p structures with a close-to-intrinsic HaP film, and the selective contacts then dictate the electric field strength throughout the HaP absorber.We thank the Yotam project, Ullmann Family Foundation, Dears Foundation, the WISâ Sustainability And Energy Research Initiative, SAERI, and the Minerva Centre for Self-Repairing Systems for Energy & Sustainability for support at the Weizmann Institute and the Israel Ministry of Energy and Infrastructure for the work at Bar-Ilan University. A.Z. thanks Katya Rechav for the FIB sample preparation, Ifat Kaplan-Asheri for assisting with EBIC operation, and Isaac Balberg (Hebrew University of Jerusalem) for fruitful discussions
How Important Is the Organic Part of Lead Halide Perovskite Photovoltaic Cells? Efficient CsPbBr<sub>3</sub> Cells
Hybrid organicâinorganic lead
halide perovskite photovoltaic
cells have already surpassed 20% conversion efficiency in the few
years that they have been seriously studied. However, many fundamental
questions still remain unanswered as to why they are so good. One
of these is âIs the organic cation really necessary to obtain
high quality cells?â In this study, we show that an all-inorganic
version of the lead bromide perovskite material works equally well
as the organic one, in particular generating the high open circuit
voltages that are an important feature of these cells
Imaging Modalities to Identity Inflammation in an Atherosclerotic Plaque
Atherosclerosis is a chronic, progressive, multifocal arterial wall disease caused by local and systemic inflammation responsible for major cardiovascular complications such as myocardial infarction and stroke. With the recent understanding that vulnerable plaque erosion and rupture, with subsequent thrombosis, rather than luminal stenosis, is the underlying cause of acute ischemic events, there has been a shift of focus to understand the mechanisms that make an atherosclerotic plaque unstable or vulnerable to rupture. The presence of inflammation in the atherosclerotic plaque has been considered as one of the initial events which convert a stable plaque into an unstable and vulnerable plaque. This paper systemically reviews the noninvasive and invasive imaging modalities that are currently available to detect this inflammatory process, at least in the intermediate stages, and discusses the ongoing studies that will help us to better understand and identify it at the molecular level
Deleterious Effect of Negative Capacitance on the Performance of Halide Perovskite Solar Cells
Negative capacitance in photovoltaic devices has been observed and reported in several cases, but its origin, at low or intermediate frequencies, is under debate. Here we unambiguously demonstrate a direct correlation between the observation of this capacitance and a corresponding decrease in performance of a halide perovskite (HaP; CsPbBr3)-based device, expressed as reduction of open-circuit voltage and fill factor. We have prepared highly stable CsPbBr3 HaPs that do not exhibit any degradation over the duration of the impedance spectroscopy measurements, ruling out degradation as the origin of the observed phenomena. Reconstruction of current-voltage curves from the impedance spectroscopy provided further evidence of the deleterious role of negative capacitance on photoconversion performance
Cesium Enhances Long-Term Stability of Lead Bromide Perovskite-Based Solar Cells
Direct comparison between perovskite-structured
hybrid organicâinorganic
methylammonium lead bromide (MAPbBr<sub>3</sub>) and all-inorganic
cesium lead bromide (CsPbBr<sub>3</sub>), allows identifying possible
fundamental differences in their structural, thermal and electronic
characteristics. Both materials possess a similar direct optical band
gap, but CsPbBr<sub>3</sub> demonstrates a higher thermal stability
than MAPbBr<sub>3</sub>. In order to compare device properties, we
fabricated solar cells, with similarly synthesized MAPbBr<sub>3</sub> or CsPbBr<sub>3</sub>, over mesoporous titania scaffolds. Both cell
types demonstrated comparable photovoltaic performances under AM1.5
illumination, reaching power conversion efficiencies of âŒ6%
with a poly aryl amine-based derivative as hole transport material.
Further analysis shows that Cs-based devices are as efficient as,
and more stable than methylammonium-based ones, after aging (storing
the cells for 2 weeks in a dry (relative humidity 15â20%) air
atmosphere in the dark) for 2 weeks, under constant illumination (at
maximum power), and under electron beam irradiation
Light-Induced Increase of Electron Diffusion Length in a pân Junction Type CH<sub>3</sub>NH<sub>3</sub>PbBr<sub>3</sub> Perovskite Solar Cell
High band gap, high open-circuit
voltage solar cells with methylammonium
lead tribromide (MAPbBr<sub>3</sub>) perovskite absorbers are of interest
for spectral splitting and photoelectrochemical applications, because
of their good performance and ease of processing. The physical origin
of high performance in these and similar perovskite-based devices
remains only partially understood. Using cross-sectional electron-beam-induced
current (EBIC) measurements, we find an increase in carrier diffusion
length in MAPbBr<sub>3</sub>(Cl)-based solar cells upon low intensity
(a few percent of 1 sun intensity) blue laser illumination. Comparing
dark and illuminated conditions, the minority carrier (electron) diffusion
length increases about 3.5 times from <i>L</i><sub>n</sub> = 100 ± 50 nm to 360 ± 22 nm. The EBIC cross section profile
indicates a pân structure between the n-FTO/TiO<sub>2</sub> and p-perovskite, rather than the pâiân structure,
reported for the iodide derivative. On the basis of the variation
in space-charge region width with varying bias, measured by EBIC and
capacitanceâvoltage measurements, we estimate the net-doping
concentration in MAPbBr<sub>3</sub>(Cl) to be 3â6 Ă 10<sup>17</sup> cm<sup>â3</sup>
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Valence and Conduction Band Densities of States of Metal Halide Perovskites: A Combined ExperimentalâTheoretical Study
We
report valence and conduction band densities of states measured
via ultraviolet and inverse photoemission spectroscopies on three
metal halide perovskites, specifically methylammonium lead iodide
and bromide and cesium lead bromide (MAPbI<sub>3</sub>, MAPbBr<sub>3</sub>, CsPbBr<sub>3</sub>), grown at two different institutions
on different substrates. These are compared with theoretical densities
of states (DOS) calculated via density functional theory. The qualitative
agreement achieved between experiment and theory leads to the identification
of valence and conduction band spectral features, and allows a precise
determination of the position of the band edges, ionization energy
and electron affinity of the materials. The comparison reveals an
unusually low DOS at the valence band maximum (VBM) of these compounds,
which confirms and generalizes previous predictions of strong band
dispersion and low DOS at the MAPbI<sub>3</sub> VBM. This low DOS
calls for special attention when using electron spectroscopy to determine
the frontier electronic states of lead halide perovskites
Low-Temperature Solution-Grown CsPbBr<sub>3</sub> Single Crystals and Their Characterization
Cesium
lead bromide (CsPbBr<sub>3</sub>) was recently introduced
as a potentially high performance thin-film halide perovskite (HaP)
material for optoelectronics, including photovoltaics, significantly
more stable than MAPbBr<sub>3</sub> (MA = CH<sub>3</sub>NH<sub>3</sub><sup>+</sup>). Because of the importance of single crystals to study
relevant material properties per se, crystals grown under conditions
comparable to those used for preparing thin films, i.e., low-temperature
solution-based growth, are needed. We show here two simple ways, antisolvent-vapor
saturation or heating a solution containing retrograde soluble CsPbBr<sub>3</sub>, to grow single crystals of CsPbBr<sub>3</sub> from a precursor
solution, treated with acetonitrile (MeCN) or methanol (MeOH). The
precursor solutions are stable for at least several months. Millimeter-sized
crystals are grown without crystal-seeding and can provide a 100%
yield of CsPbBr<sub>3</sub> perovskite crystals, avoiding a CsBr-rich
(or PbBr<sub>2</sub>-rich) composition, which is often present alongside
the perovskite phase. Further growth is demonstrated to be possible
with crystal seeding. The crystals are characterized in several ways,
including first results of charge carrier lifetime (30 ns) and an
upper-limit of the Urbach energy (19 meV). As the crystals are grown
from a polar aprotic solvent (DMSO), which is similar to those used
to grow hybrid organicâinorganic HaP crystals, this may allow
growing mixed (organic and inorganic) monovalent cation HaP crystals