Publication date: 1st July 2014
Organic-inorganic hybrid semiconductors based on metal halide units have attracted attention due to their interesting structural and optical properties. In particular, attention has been focused on the 2D-layered organic-inorganic perovskite semiconductors (R-NH3)2PbX4 with R an organic group and X the halide (Cl-, Br-, I-) because of their application in emitting optical devices [1,2] and recently on 3D perovskites such as CH3NH3PbX3 which reveal particularly convenient for the photovoltaïc applications [3-5]. Among several advantages, these materials are remarkable due to their excitonic properties: for example the 2D perovskites form self-assembled ordered quantum well structures, in which the excitons are strongly confined in the very thin inorganic wells PbX62-, resulting in a very large exciton binding energy of a few hundred of meV. Understanding the nature of the excitons in perovskites is crucial to optimize the opto-electronic devices, the emitting ones requiring strong excitons at room temperature as well as the absorbing ones where the exciton has to be separated to generate free carriers.
We focus here our attention on 2D mixed perovskites (C6H5-C2H4-NH3)2PbZ4(1-x)Y4x, and 3D mixed perovskites CH3NH3PbZ3-xYx where Z, Y = I, Br or Cl. Firstly, we show that 2D and 3D mixed perovskites afford similar continuous optical tunability at room temperature. Secondly, studying experimentally the disorder induced effects on the optical properties, we demonstrate that they can be considered as pseudobinary alloys, exactly like Ga1-xAlxAs, Cd1-xHgxTe inorganic semiconductors. We develop a theoretical analysis which allows to describe the influence of alloying on the excitonic properties of perovskite molecular crystals. Despite a large binding energy of several 100 meV, the 2D excitons present a Wannier character rather than a Frenkel character. The small inhomogeneous broadening reported in 3D hybrid alloyed compounds is similarly consistent with delocalized electron hole pairs at room temperature rather than strongly localized excitons.
References:
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[2] G. Lanty, J.S. Lauret, D. Byrne, E. Deleporte, S. Bouchoule and X. Lafosse, Appl. Phys. Lett. 93, 81101 (2008)
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