Strongly bound excitons in Ruddlesden-Popper 2D perovskites

ORAL

Abstract

Ruddlesden-Popper halide perovskites are 2D solution-processed quantum wells with a general formula A2A’n-1MnX3n+1, where A, A’ are cations, M is a metal, X is a halide, and their physical properties can be tuned by varying the perovskite layer thickness (n value). They have recently emerged as efficient semiconductors for optoelectronics [1-3]. However, fundamental questions concerning the nature of optical resonances, their scaling with quantum well thickness, and the physics behind the exciton properties, remain unresolved. Here, using optical spectroscopy and 60-Tesla magneto-absorption supported by modelling, we unambiguously demonstrate that the optical resonances arise from tightly bound excitons with binding energies varying from 470 meV to 125 meV with increasing thickness from n=1 to 5 [4]. Comprehensive modelling of exciton states enable the understanding of dielectric confinement effects which prevail over quantum confinement in 2D perovskites. From these results we produce a general scaling behaviour for the binding energy of exciton states in Ruddlesden-Popper perovskites.

[1] Tsai et al., Nature (2016), 536, 312-316.
[2] M. Yuan et al., Nat. Nanotechnol. (2016), 11, 872-877.
[3] Blancon et al., Science (2017), 355, 1288-1292.
[4] Blancon et al., arXiv:1710.07653.

Presenters

  • Jean-Christophe Blancon

    Los Alamos National Laboratory, Materials Physics and Applications Division, Los Alamos National Laboratory

Authors

  • Jean-Christophe Blancon

    Los Alamos National Laboratory, Materials Physics and Applications Division, Los Alamos National Laboratory

  • Andreas Steir

    Los Alamos National Laboratory

  • Wanyi Nie

    Los Alamos National Laboratory, Los Alamos National Lab, Materials Physics and Applications Division, Los Alamos National Laboratory

  • Hsinhan Tsai

    Rice University, Los Alamos National Lab

  • Constantinos Stoumpos

    Northwestern University

  • Scott Crooker

    National High Magnetic Field Laboratory, Los Alamos National Laboratory, National High Magnetic Field Laboratory, Los Alamos National Lab, Los Alamos National Laboratory, NHMFL, Los Alamos National Laboratory

  • Mercouri Kanatzidis

    Department of Chemistry, Northwestern University, Materials Science Division, Argonne National Laboratory, Northwestern Univ, Materials Science Division, Argonne Natl Lab, Northwestern University

  • Jared Crochet

    Los Alamos National Laboratory

  • Jacky Even

    INSA FOTON, INSA de Rennes, Université de Rennes 1, Fonctions Optiques pour les Technologies de l’Information (FOTON), Institut National des Sciences Appliquées (INSA) de Rennes, CNRS, UMR 6082

  • Aditya Mohite

    MPA-11: Materials Synthesis and Integrated Devices, Los Alamos National Laboratory, Los Alamos National Laboratory, Los Alamos National Lab, Materials Physics and Applications Division, Los Alamos National Laboratory