4.8 Article

Giant Electron-Phonon Coupling and Deep Conduction Band Resonance in Metal Halide Double Perovskite

Journal

ACS NANO
Volume 12, Issue 8, Pages 8081-8090

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acsnano.8b02936

Keywords

double perovskite; Cs2AgBiBr6; Frohlich interactions; Raman scattering; conduction band resonance

Funding

  1. Research Foundation-Flanders (FWO) [G.0962.13, G.0B39.15, G.0197.11, ZW15_09 GOH6316]
  2. KU Leuven Research Fund [C14/15/053]
  3. Flemish government through long term structural funding Methusalem (CASAS2) [Meth/15/04]
  4. Hercules foundation [HER/11/14]
  5. Belgian Federal Science Policy Office [IAP-VII/05]
  6. European Research Council under the European Union's Seventh Framework Programme (FP/2007-2013)/ERC grant [307523]
  7. ERC-Stg LIGHT

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The room-temperature charge carrier mobility and excitation emission properties of metal halide perovskites are governed by their electronic band structures and intrinsic lattice phonon scattering mechanisms. Establishing how charge carriers interact within this scenario will have far-reaching consequences for developing high-efficiency materials for optoelectronic applications. Herein we evaluate the charge carrier scattering properties and conduction band environment of the double perovskite Cs2AgBiBr6 via a combinatorial approach; single crystal X-ray diffraction, optical excitation and temperature-dependent emission spectroscopy, resonant and nonresonant Raman scattering, further supported by first-principles calculations. We identify deep conduction band energy levels and that scattering from longitudinal optical phonons-via the Frohlich interaction-dominates electron scattering at room temperature, manifesting within the nominally nonresonant Raman spectrum as multiphonon processes up to the fourth order. A Frohlich coupling constant nearing 230 meV is inferred from a temperature-dependent emission line width analysis and is found to be extremely large compared to popular lead halide perovskites (between 40 and 60 meV), highlighting the fundamentally different nature of the two single and double perovskite materials branches.

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