Fine structure of excitons and electron–hole exchange energy in polymorphic CsPbBr3 single nanocrystals. Issue 14 (21st March 2018)

• Record Type: Journal Article
• Authors: Ramade, Julien; Andriambariarijaona, Léon Marcel; Steinmetz, Violette; Goubet, Nicolas; Legrand, Laurent; Barisien, Thierry; Bernardot, Frédérick; Testelin, Christophe; Lhuillier, Emmanuel; Bramati, Alberto; Chamarro, Maria
• Is Part Of: Nanoscale. Volume 10:Issue 14(2018)
• Page Start: 6393
• Page End: 6401
• Publication Date: 2018-03-21
• Subjects: Nanoscience -- Periodicals; Nanotechnology -- Periodicals; 620.505
• DOI: 10.1039/c7nr09334a
• Languages: English
• ISSNs: 2040-3364

Abstract

Abstract : Electron–hole exchange energy, J, rules the exciton fine structure splittings in CsPbBr3 single nanocrystals. Abstract : All inorganic CsPbX3 (X = Cl, Br, I) nanocrystals (NCs) belong to the novel class of confined metal–halide perovskites which are currently arousing enthusiasm and stimulating huge activity across several fields of optoelectronics due to outstanding properties. A deep knowledge of the band-edge excitonic properties of these materials is thus crucial to further optimize their performances. Here, high-resolution photoluminescence (PL) spectroscopy of single bromide-based NCs reveals the exciton fine structure in the form of sharp peaks that are linearly polarized and grouped in doublets or triplets, which directly mirror the adopted crystalline structure, tetragonal ( D 4h symmetry) or orthorhombic ( D 2h symmetry). Intelligible equations are found that show how the fundamental parameters (spin–orbit coupling, Δ SO, crystal field term, T, and electron–hole exchange energy, J ) rule the energy spacings in doublets and triplets. From experimental data, fine estimations of each parameter are obtained. The analysis of the absorption spectra of an ensemble of NCs with a "quasi-bulk" behavior leads to Δ SO = 1.20 ± 0.06 eV and T = −0.34 ± 0.05 eV in CsPbBr3 . The study of individual luminescence responses of NCs having sizes comparable to the exciton Bohr diameter, 7 nm, allows us to estimate the value of J to be around ≈3 meV in both tetragonal and orthorhombic phases. This value is already enhanced by confinement.