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Reversible Hydration of CH3NH3PbI3 in Films, Single Crystals, and Solar Cells

TLDR
In this paper, it was shown that hydrated crystal phases are formed when methylammonium lead iodide perovskite (MAPI) is exposed to water vapor at room temperature and these phase changes are fully reversed when the material is subsequently dried.
Abstract
Solar cells composed of methylammonium lead iodide perovskite (MAPI) are notorious for their sensitivity to moisture. We show that (i) hydrated crystal phases are formed when MAPI is exposed to water vapor at room temperature and (ii) these phase changes are fully reversed when the material is subsequently dried. The reversible formation of CH3NH3PbI3·H2O followed by (CH3NH3)4PbI6·2H2O (upon long exposure times) was observed using time-resolved XRD and ellipsometry of thin films prepared using “solvent engineering”, single crystals, and state-of-the-art solar cells. In contrast to water vapor, the presence of liquid water results in the irreversible decomposition of MAPI to form PbI2. MAPI changes from dark brown to transparent on hydration; the precise optical constants of CH3NH3PbI3·H2O formed on single crystals were determined, with a bandgap at 3.1 eV. Using the single-crystal optical constants and thin-film ellipsometry measurements, the time-dependent changes to MAPI films exposed to moisture were m...

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Journal ArticleDOI

Organic–Inorganic Perovskites: Structural Versatility for Functional Materials Design

TL;DR: This review will explore beyond the current focus on three-dimensional (3-D) lead(II) halide perovskites, to highlight the great chemical flexibility and outstanding potential of the broader class of 3-D and lower dimensional organic-based perovSKite family for electronic, optical, and energy-based applications as well as fundamental research.
Journal ArticleDOI

Halide Perovskite Photovoltaics: Background, Status, and Future Prospects

TL;DR: The fundamentals, recent research progress, present status, and views on future prospects of perovskite-based photovoltaics, with discussions focused on strategies to improve both intrinsic and extrinsic (environmental) stabilities of high-efficiency devices are described.
Journal ArticleDOI

One-Year stable perovskite solar cells by 2D/3D interface engineering

TL;DR: One-year stable perovskite devices are shown by engineering an ultra-stable 2D/3D (HOOC(CH2)4NH3)2PbI4/CH3NH3Pb mezzanine junction, which will enable the timely commercialization of perovSKite solar cells.
Journal ArticleDOI

Stabilizing Perovskite Structures by Tuning Tolerance Factor: Formation of Formamidinium and Cesium Lead Iodide Solid-State Alloys

TL;DR: In this article, the effect of alloying FA0.85Cs0.15PbI3 with CsPbIsI3 was investigated, and it was shown that the effective tolerance factor can be tuned and the stability of the photoactive α-phase of the mixed solid-state perovskite alloys FA1-xCsxPbisI3 is enhanced.
Journal ArticleDOI

Organometal halide perovskite solar cells: degradation and stability

TL;DR: In this paper, the causes of failure and associated mechanisms of device degradation, approaches to improve stability, and methods and protocols are discussed in detail and form the main focus of the review article.
References
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Journal ArticleDOI

Organometal Halide Perovskites as Visible-Light Sensitizers for Photovoltaic Cells

TL;DR: Two organolead halide perovskite nanocrystals were found to efficiently sensitize TiO(2) for visible-light conversion in photoelectrochemical cells, which exhibit strong band-gap absorptions as semiconductors.
Journal ArticleDOI

Interface engineering of highly efficient perovskite solar cells

TL;DR: Perovskite films received a boost in photovoltaic efficiency through controlled formation of charge-generating films and improved current transfer to the electrodes and low-temperature processing steps allowed the use of materials that draw current out of the perovskites layer more efficiently.
Journal ArticleDOI

Chemical Management for Colorful, Efficient, and Stable Inorganic–Organic Hybrid Nanostructured Solar Cells

TL;DR: This paper demonstrates highly efficient solar cells exhibiting 12.3% in a power conversion efficiency of under standard AM 1.5, for the most efficient device, as a result of tunable composition for the light harvester in conjunction with a mesoporous TiO2 film and a hole conducting polymer.
Journal ArticleDOI

Low trap-state density and long carrier diffusion in organolead trihalide perovskite single crystals

TL;DR: An antisolvent vapor-assisted crystallization approach is reported that enables us to create sizable crack-free MAPbX3 single crystals with volumes exceeding 100 cubic millimeters, which enabled a detailed characterization of their optical and charge transport characteristics.
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Frequently Asked Questions (18)
Q1. What have the authors contributed in "The reversible hydration of ch3nh3pbi3 in films, single crystals and solar cells" ?

The authors show that hydrated crystal phases are formed when MAPI is exposed to water vapour at room temperature and that these phase changes are fully reversed when the material is subsequently dried. The reversible formation of CH3NH3PbI3•H2O followed by ( CH3NH3 ) 4PbI6•2H2O ( upon long exposure times ) was observed using time resolved XRD and ellipsometry of thin films prepared using ‘ solvent engineering ’, single crystals, and state of the art solar cells. Hysteresis in the current-voltage characteristics was significantly increased after this dehydration, which may be related to changes in the defect density and morphology of MAPI following recrystallization from the hydrate. The results suggest that the mono-hydrate phase forms independently of the depth in the film suggesting rapid transport of water molecules along grain boundaries. Vapour phase hydration of an unencapsulated solar cell ( initially Jsc ≈ 19 mA cm -2 and Voc ≈ 1. 05 V at 1 sun ) resulted in more than a 90 % drop in short circuit photocurrent and around 200 mV loss in open circuit potential, but these losses were fully reversed after the cell was exposed to dry nitrogen for 6 hours. Based on their observations the authors suggest that irreversible decomposition of MAPI in the presence of water vapour only occurs significantly once a grain has been fully converted to the hydrate phase. 

After 30 s total spinning time, the substrate was immediately annealed at 100 °C for 10 min to evaporate residual solvents and to further promote crystallization. 

Since the presence of water vapour appears to catalyse dynamic recrystalisation within the film between the hydrated and pure crystalline phases, this may lead to higher quality films under the optimised processing conditions as long as water is subsequently completely removed by thermal annealing. 

To complete the transformation of TiOx into the anatase phase, the coated substrates were gradually heated to 500 °C (ramp 8 °C/min) and sintered for 45 min in air. 

The release of water as the reaction goes from the monohydrate to the dihydrate suggests partial self-sustainability of the conversion process as the water molecules released can be reused to convert remaining MAPI into the monohydrate. 

3Ensuring the stability of MAPI photovoltaics under operational conditions is one of the biggest barriers to commercializing the technology. 

The product obtained was metastable and turned into greyish polycrystalline MAPI by spontaneous loss of its crystalline water under ambient conditions. 

a 40 nm thick gold layer was deposited by thermal evaporation through a patterned shadow mask under high vacuum conditions (4 × 10-6 mbar) to form the counter electrode. 

Ellipsometry spectra were recorded every 10 or 20minutes during the conversion of a crystalline MAPI film to CH3NH3PbI3•H2O by exposure to air with RH 80 % over a period of 100 minutes. 

The three fit parameters in this model are: the thickness of the solid thin film, the thickness of the roughness layer on top of the film, and the relative ratio of MAPI and its hydrate in the mixture forming the film and roughness layer. 

The reduction of this peak intensity is accompanied by a decrease of the peak intensities associated with MAPI monohydrates and a concomitant increase in the intensity of the crystalline MAPI peaks. 

14,15 Using the fitted hydrate content as a function of exposure time (Figure 3 in the main text), values of the increase of the solid layer thickness due to its expansion on partial hydration can be estimated. 

The substrates were coated with the TiOx sol-gel solution by spin-coating dynamically at 2000 rpm for 45 s and then quickly placed on a hotplate at 150 °C for 10 min. 

Surface roughness between two layers is also commonly described by an EMA layer consisting of a composite of top and bottom material in equal proportion. 

The authors observed that for crystallites of similar sizes, dehydration appears to be a faster process that hydration at room temperature. 

Although not yet widely appreciated, MAPI clearly shows a propensity to form new solvated crystal structures at room temperature by incorporating small polar molecules. 

It is apparent for both scan directions that there is almost an order of magnitude drop in the photocurrent and around a 200 mV loss in photovoltage after the device was exposed to moisture for 3 hours. 

Dihydrate crystals are obtained –together with the monohydrate species– in directly synthesized hydrated MAPI needle shaped crystals prepared from solution (methods section, photographs in Figure S4, characteristic reflection at 2θ = 11.39° in XRD pattern in Figure 2a).