Phase Diagram of Methylammonium/Formamidinium Lead Iodide Perovskite Solid Solutions from Temperature-Dependent Photoluminescence and Raman Spectroscopies

The complete phase diagram of organic-cation solid solutions of lead iodide perovskites [FAxMA1–xPbI3, where MA stands for methylammonium, CH3NH3, and FA for formamidinium, CH(NH2)2] with compositions x ranging from 0 to 1 in steps of 0.1 was constructed in the temperature range from 10 to 365 K by...

Full description

Bibliographic Details
Authors: Francisco López, Adrián, Charles, Bethan, Alonso Carmona, M. Isabel, Garriga Bacardi, Miquel, Campoy Quiles, Mariano, Weller, Mark T., Goñi, Alejandro R.
Format: article
Status:Versión aceptada para publicación
Publication Date:2020
Country:España
Institution:Consejo Superior de Investigaciones Científicas (CSIC)
Repository:DIGITAL.CSIC. Repositorio Institucional del CSIC
OAI Identifier:oai:digital.csic.es:10261/210417
Online Access:http://hdl.handle.net/10261/210417
Access Level:Open access
Keyword:Halide perovskites
Optical-properties
Single-crystals
Organic cations
Formadinium
Description
Summary:The complete phase diagram of organic-cation solid solutions of lead iodide perovskites [FAxMA1–xPbI3, where MA stands for methylammonium, CH3NH3, and FA for formamidinium, CH(NH2)2] with compositions x ranging from 0 to 1 in steps of 0.1 was constructed in the temperature range from 10 to 365 K by combining Raman scattering and photoluminescence (PL) measurements. The occurrence of phase transitions was inferred from both the temperature-induced changes in the optical emission energies and/or the phonon frequencies and line widths, complementing X-ray and neutron scattering literature data. For MA-rich perovskites (x ≤ 0.2), the same structural behavior as for MAPbI3 was observed with decreasing temperature: cubic Pm3̅m → tetragonal-I I4/mcm → orthorhombic Pnma. As the FA molecule is larger and more symmetric but less polar than MA, a tetragonal crystal structure is favored at low temperatures and FA compositions x > 0.4, to the detriment of the orthorhombic phase. As a consequence, with decreasing temperature, the phase transition sequence for FA-rich compounds is cubic Pm3̅m → tetragonal-II P4/mbm → tetragonal-III. The latter presumably belongs to the P4bm symmetry group, according to neutron scattering data. Strikingly, the isostructural (tetragonal-to-tetragonal) transformation, which occurs between 200 and 150 K, exhibits a kind of critical point for x = 0.7. For intermediate FA contents, the perovskite solid solution transforms close to 250 K directly from the cubic phase to the tetragonal-III phase. The latter is characterized by a nonmonotonic dependence of the band-gap energy on temperature. We ascribe such behavior to a substantial tilting of the PbI6 octahedra in the tetragonal-III phase. In this way, we established important links between crystal-phase stability and the electronic as well as vibrational properties of mixed organic-cation halide perovskites, which might impact the current search for more stable best-performing optoelectronic materials.