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      Quasi‐2D Perovskite Crystalline Layers for Printable Direct Conversion X‐Ray Imaging

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          High-efficiency two-dimensional Ruddlesden–Popper perovskite solar cells

          Three-dimensional organic-inorganic perovskites have emerged as one of the most promising thin-film solar cell materials owing to their remarkable photophysical properties, which have led to power conversion efficiencies exceeding 20 per cent, with the prospect of further improvements towards the Shockley-Queisser limit for a single‐junction solar cell (33.5 per cent). Besides efficiency, another critical factor for photovoltaics and other optoelectronic applications is environmental stability and photostability under operating conditions. In contrast to their three-dimensional counterparts, Ruddlesden-Popper phases--layered two-dimensional perovskite films--have shown promising stability, but poor efficiency at only 4.73 per cent. This relatively poor efficiency is attributed to the inhibition of out-of-plane charge transport by the organic cations, which act like insulating spacing layers between the conducting inorganic slabs. Here we overcome this issue in layered perovskites by producing thin films of near-single-crystalline quality, in which the crystallographic planes of the inorganic perovskite component have a strongly preferential out-of-plane alignment with respect to the contacts in planar solar cells to facilitate efficient charge transport. We report a photovoltaic efficiency of 12.52 per cent with no hysteresis, and the devices exhibit greatly improved stability in comparison to their three-dimensional counterparts when subjected to light, humidity and heat stress tests. Unencapsulated two-dimensional perovskite devices retain over 60 per cent of their efficiency for over 2,250 hours under constant, standard (AM1.5G) illumination, and exhibit greater tolerance to 65 per cent relative humidity than do three-dimensional equivalents. When the devices are encapsulated, the layered devices do not show any degradation under constant AM1.5G illumination or humidity. We anticipate that these results will lead to the growth of single-crystalline, solution-processed, layered, hybrid, perovskite thin films, which are essential for high-performance opto-electronic devices with technologically relevant long-term stability.
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            Solar cells. High-efficiency solution-processed perovskite solar cells with millimeter-scale grains.

            State-of-the-art photovoltaics use high-purity, large-area, wafer-scale single-crystalline semiconductors grown by sophisticated, high-temperature crystal growth processes. We demonstrate a solution-based hot-casting technique to grow continuous, pinhole-free thin films of organometallic perovskites with millimeter-scale crystalline grains. We fabricated planar solar cells with efficiencies approaching 18%, with little cell-to-cell variability. The devices show hysteresis-free photovoltaic response, which had been a fundamental bottleneck for the stable operation of perovskite devices. Characterization and modeling attribute the improved performance to reduced bulk defects and improved charge carrier mobility in large-grain devices. We anticipate that this technique will lead the field toward synthesis of wafer-scale crystalline perovskites, necessary for the fabrication of high-efficiency solar cells, and will be applicable to several other material systems plagued by polydispersity, defects, and grain boundary recombination in solution-processed thin films.
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              Sensitive X-ray detectors made of methylammonium lead tribromide perovskite single crystals

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                Author and article information

                Contributors
                Journal
                Advanced Materials
                Advanced Materials
                Wiley
                0935-9648
                1521-4095
                April 2022
                February 19 2022
                April 2022
                : 34
                : 13
                : 2106498
                Affiliations
                [1 ]Center for Integrated Nanotechnologies Los Alamos National Laboratory Los Alamos NM 87544 USA
                [2 ]Department of Chemistry University of California, Berkeley Berkeley CA 94720 USA
                [3 ]Nuclear Engineering Program Department of Mechanical and Aerospace Engineering The Ohio State University Columbus OH 43210 USA
                [4 ]Center for Condensed Matter Sciences National Taiwan University No. 1, Sec. 4, Roosevelt Rd. Taipei 10617 Taiwan
                [5 ]Department of Material Science and Engineering National Taiwan University No. 1, Sec. 4, Roosevelt Rd. Taipei 10617 Taiwan
                [6 ]X‐Ray Science Division Argonne National Laboratory Lemont IL 60439 USA
                Article
                10.1002/adma.202106498
                35106838
                14eaeafe-90c6-4955-b593-f8b0c3cc53c3
                © 2022

                http://creativecommons.org/licenses/by-nc-nd/4.0/

                http://doi.wiley.com/10.1002/tdm_license_1.1

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