4.8 Article

Interfacial Electromechanics Predicts Phase Behavior of 2D Hybrid Halide Perovskites

Journal

ACS NANO
Volume 14, Issue 3, Pages 3353-3364

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acsnano.9b09105

Keywords

2D hybrid organic-inorganic perovskite; interfacial dipole; multiscale modeling; critical phase behavior; surface stress

Funding

  1. Army Research Office [W911NF-16-1-0447]
  2. U.S. National Science Foundation [EFMA-542879, CMMI-1727717]
  3. [2022-1652]

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Quasi-two-dimensional (2D) mixed-cation hybrid halide perovskites (A' (2)A(N-1)M(N)X(3N-r); A' = large organic molecule with cationic group, A = [Cs+, CH3NH3+, HC-(NH2)(2)], M = [Pb, Sn, Ge], X = [I-, Br-, Cl-]) have rapidly emerged as candidates to improve the structural stability and device lifetime of 3D perovskite semiconductor devices under operating conditions. The addition of the large A' cation to the traditional AMX(3) structure introduces several synthetic degrees of freedom and breaks M-X bonds, giving rise to peculiar critical phase behavior in the phase space of these complex materials. In this work, we propose a thermodynamic model parametrized by first-principles calculations to generate the phase diagram of 2D and quasi-2D perovskites (q-2DPKs) based on the mechanics and electrostatics of the interface between the A' cations and the metal halide octahedral network. Focusing on the most commonly studied methylammonium lead iodide system where A' is n-butylammonium (BA; CH3(CH2)(3)NH3+), we find that the apparent difficulty in synthesizing phase-pure samples with a stoichiometric index N > 5 can be attributed to the energetic competition between repulsion of opposing interfacial dipole layers and mechanical relaxation induced by interfacial stress. Our model shows quantitative agreement with experimental observations of the maximum phase-pure stoichiometric index (N-crit) and explains the nonmonotonic evolution of the lattice parameters with increasing stoichiometric index (N). This model is generalizable to the entire family of q-2DPKs and can guide the design of photovoltaic and optical materials that combine the structural stability of the q-2DPKs while retaining the charge carrier properties of their 3D counterparts.

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