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      How to GIWAXS: Grazing Incidence Wide Angle X‐Ray Scattering Applied to Metal Halide Perovskite Thin Films

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          Abstract

          The frequency of reports utilizing synchrotron‐based grazing incident wide angle X‐ray scattering (GIWAXS) to study metal halide perovskite thin films has exploded recently, as this technique has proven invaluable for understanding several structure‐property relationships that fundamentally limit optoelectronic performance. The GIWAXS geometry and temporal resolution are also inherently compatible with in situ and operando setups (including ISOS protocols), and a relatively large halide perovskite research community has deployed GIWAXS to unravel important kinetic and dynamic features in these materials. Considering its rising popularity, the aim here is to accelerate the required learning curve for new experimentalists by clearly detailing the underlying analytical concepts which can be leveraged to maximize GIWAXS studies of polycrystalline thin films and devices. Motivated by the vast range of measurement conditions offered, together with the wide variety of compositions and structural motifs available (i.e., from single‐crystal and polycrystalline systems, to quantum dots and layered superlatices), a comprehensive framework for conducting effective GIWAXS experiments is outlined for different purposes. It is anticipated that providing a clear perspective for this topic will help elevate the quality of future GIWAXS studies—which have become routine—and provide the impetus required to develop novel GIWAXS approaches to resolve unsettled scientific questions.

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          Recent advances in magnetic structure determination by neutron powder diffraction

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            Electron-hole diffusion lengths exceeding 1 micrometer in an organometal trihalide perovskite absorber.

            Organic-inorganic perovskites have shown promise as high-performance absorbers in solar cells, first as a coating on a mesoporous metal oxide scaffold and more recently as a solid layer in planar heterojunction architectures. Here, we report transient absorption and photoluminescence-quenching measurements to determine the electron-hole diffusion lengths, diffusion constants, and lifetimes in mixed halide (CH3NH3PbI(3-x)Cl(x)) and triiodide (CH3NH3PbI3) perovskite absorbers. We found that the diffusion lengths are greater than 1 micrometer in the mixed halide perovskite, which is an order of magnitude greater than the absorption depth. In contrast, the triiodide absorber has electron-hole diffusion lengths of ~100 nanometers. These results justify the high efficiency of planar heterojunction perovskite solar cells and identify a critical parameter to optimize for future perovskite absorber development.
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              Commentary: The Materials Project: A materials genome approach to accelerating materials innovation

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                Author and article information

                Contributors
                (View ORCID Profile)
                Journal
                Advanced Energy Materials
                Advanced Energy Materials
                1614-6832
                1614-6840
                July 2023
                June 11 2023
                July 2023
                : 13
                : 27
                Affiliations
                [1 ] Australian Institute for Bioengineering and Nanotechnology The University of Queensland Brisbane Queensland 4072 Australia
                [2 ] School of Mathematics and Physics The University of Queensland Brisbane Queensland 4072 Australia
                [3 ] cMACS Department of Microbial and Molecular Systems KU Leuven Leuven 3001 Belgium
                [4 ] NCD‐SWEET beamline ALBA Synchrotron Light Source Cerdanyola del Vallès Barcelona 08290 Spain
                [5 ] Department of Physics Biomolecular and Organic Electronics Chemistry and Biology (IFM) Linköping University Linköping 58183 Sweden
                [6 ] Materials Science and Engineering Program University of Colorado Boulder Boulder CO 80309 USA
                [7 ] Department of Chemistry KU Leuven Celestijnenlaan 200F Leuven 3001 Belgium
                [8 ] Max Plank Institute for Polymer Research D‐55128 Mainz Germany
                [9 ] Swiss‐Norwegian Beamlines at the European Synchrotron Radiation Facility 71 Avenue des Martyrs Grenoble F‐38000 France
                [10 ] Renewable and Sustainable Energy Institute (RASEI) University of Colorado Boulder Boulder CO 80309 USA
                Article
                10.1002/aenm.202300760
                98204982-a016-4e32-a831-c5912defc54b
                © 2023

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

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

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