The Reversible Hydration of CH3NH3PbI3 in Films, Single Crystals and Solar Cells
Piers R. F. Barnes a, Aurélien M. A. Leguy a, Jenny Nelson a, Andrew McMahon a, Nicholas M. Harrison a, Pablo Docampo b, Thomas Bein b, Yinghong Hu b, M. Isabel Alonso c, Mariano Campoy-Quiles c, Mark T. Weller d, Oliver J. Weber d, Mark van Schilfgaarde e, Pooya Azarhoosh e
a Imperial College London, United Kingdom, South Kensington, Londres, Reino Unido, United Kingdom
b Ludwig-Maximilians-Universität, Professor-Huber-Platz 2, München, 80539
c University of Bath, Bath BA2 7AY, United Kingdom, United Kingdom
d Kings College London, Strand, London, United Kingdom
Materials for Sustainable Development Conference (MATSUS)
Proceedings of nanoGe September Meeting 2015 (NFM15)
Santiago de Compostela, Spain, 2015 September 6th - 15th
Oral, Aurélien M. A. Leguy, presentation 223
Publication date: 8th June 2015

Solar cells composed of methylammonium lead iodide perovskite (MAPI) are notorious for their sensitivity to moisture. We show using in situ spectroscopic ellipsometry and X-ray diffraction of thin films, single crystals and solar cells: (i) Hydrated crystal phases are formed when MAPI is exposed to water vapour at room temperature. (ii) These phase changes are reversed when the material is subsequently dried. The reversible hydration/dehydration in the presence/absence of water vapour appears to proceed via: 

4 (CH3NH3)PbI3 + 4 H2O ⇌ 4 [CH3NH3PbI3•H2O] ⇌(CH3NH3)4PbI6•2H2O + 3 PbI2 + 2 H2

In contrast to water vapour, 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, and are discussed in the context of DFT calculations of the structures. 

Using the single-crystal optical constants and thin-film ellipsometry measurements, the time-dependent changes to MAPI films exposed to moisture were modelled. The results suggest that the monohydrate phase forms independent of the depth in the film, suggesting rapid transport of water molecules along grain boundaries. Vapour-phase hydration of an un-encapsulated 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 ∼200 mV loss in open-circuit potential; however, these losses were fully reversed after the device was exposed to dry nitrogen for 6 h. 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. Based on our observations, we suggest that irreversible decomposition of MAPI in the presence of water vapour only occurs significantly once a grain has been fully converted to the monohydrate phase. 



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