Orientational Glass Formation in Substituted Hybrid Perovskites

Eve M. Mozur, Annalise E. Maughan, Yongqiang Cheng, Ashfia Huq, Niina Jalarvo, Luke L. Daemen, James R. Neilson

Research output: Contribution to journalArticlepeer-review

42 Scopus citations

Abstract

Hybrid organic-inorganic perovskites have gained notoriety in the photovoltaic community for their composition-tunable band gaps and long-lived electronic excited states, which are known to be related to the crystalline phase. While it is known that the inorganic and organic components are coupled through structural phase transitions, it remains unclear as to what role each plays in directing the structure of hybrid perovskites such as methylammonium lead halides (CH3NH3PbX3). Here, we present crystallographic and spectroscopic data for the series (CH3NH3)1-xCsxPbBr3. CH3NH3PbBr3 behaves as a plastic crystal in the high temperature cubic phase, and substitution of CH3NH3+ with Cs+ leads to the formation of an orientational glass. While the organic molecule exhibits slow, glassy reorientational dynamics, the inorganic framework continues to undergo crystallographic phase transitions. These crystallographic transitions occur in the absence of thermodynamic signatures in the specific heat from molecular orientation transitions, which suggests that the phase transitions result from underlying instabilities intrinsic to the inorganic lattice. However, these transitions are not decoupled from the reorientations of the organic molecule, as indicated by inelastic and quasielastic neutron scattering. Observation of a reentrant phase transition in (CH3NH3)0.8Cs0.2PbBr3 permits the resolution of these complex behaviors within the context of strain mediated interactions. Together, these results provide critical insight into the coupled phase behavior and dynamics in hybrid perovskites.

Original languageEnglish
Pages (from-to)10168-10177
Number of pages10
JournalChemistry of Materials
Volume29
Issue number23
DOIs
StatePublished - Dec 12 2017

Funding

This work at Colorado State University was supported by the U.S. Department of Energy, Office of Science, Basic Energy Sciences, under Award SC0016083. A portion of this research used resources at the Spallation Neutron Source, a DOE Office of Science User Facility operated by the Oak Ridge National Laboratory. The computing resources for the phonon and INS calculations were made available through the VirtuES and ICEMAN projects, funded by the Laboratory Directed Research and Development program at Oak Ridge National Laboratory. Use of the Advanced Photon Source at Argonne National Laboratory was supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357. The authors would also like to thank Dr. K. A. Ross for many helpful discussions and the reviewers for their insightful comments. This work at Colorado State University was supported by the U.S. Department of Energy, Office of Science, Basic Energy Sciences under Award SC0016083. A portion of this research used resources at the Spallation Neutron Source, a DOE Office of Science User Facility operated by the Oak Ridge National Laboratory. The computing resources for the phonon and INS calculations were made available through the VirtuES and ICEMAN projects, funded by the Laboratory Directed Research and Development program at Oak Ridge National Laboratory. Use of the Advanced Photon Source at Argonne National Laboratory was supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357.

FundersFunder number
Office of Basic Energy Sciences
U.S. Department of Energy
Office of Science
Basic Energy SciencesSC0016083
Argonne National Laboratory
Oak Ridge National Laboratory
Colorado State University

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