Proceedings of International Conference on Perovskite Thin Film Photovoltaics, Photonics and Optoelectronics (ABXPV18PEROPTO)
DOI: https://doi.org/10.29363/nanoge.abxpvperopto.2018.058
Publication date: 11th December 2017
We investigate the exciton fine structure (EFS) and exciton-phonon coupling (EPC) of individual CsPbBr3 nanocrystals (NCs). These NCs belong to the novel class of confined inorganic metal-halide perovkites that currently arouses enthusiasm and stimulates a huge activity due to its outstanding attendant properties within several fields of optoelectronics. The NCs studied in this work are synthesized in a form of colloidal solution through a previously described method [1] and present a cubic shape, which length dispersion is very sensitive to the temperature synthesis.
Micro-photoluminescence (μ-PL) measurements at cryogenic temperature reveal an EFS composed by either two or three Lorentzian-shaped ultrasharp peaks, which directly mirrors the adopted crystalline structure [2], namely tetragonal (doublet) or orthorhombic (triplet). We show through polarization-resolved μ-PL that these peaks are orthogonally polarized. Fine analysis of the energy structure allows to determine both exchange energy terms and crystal field terms for both structure, as well as an estimation of the dark state position in the EFS.
In a second time, EPC is studied in single polymorphic NCs. For this purpose, we perform for the first time μ-PL measurements on selectively polarized lines under various temperature from 4K to 80K. The temperature-dependence of emission linewidth follows the empirical Bose-Einstein model [3], which accounts for charge-phonon coupling for both acoustic and LO (Fröhlich) phonons. We find that acoustic coupling dominates the low temperature regime (up to 30K) while in the higher temperatures, broadening is mainly ruled by the Fröhlich term.
Our results bring fundamental information for the understanding of the CsPbBr3 excitonic response as single emitters and provide new insights into their optical properties and performances for future integration in devices such as quantum sources.
[1] L. Protesescu, S. Yakunin, M.I. Bodnarchuk et al., Nano Lett. 15, 3692 (2015)
[2] M. Fu, P. Tamarat, H. Huang et al., Nano Lett. 17, 2895 (2017)
[3] S. Rudin, T.L. Reinecke and B. Segall, Phys. Rev. B. 42, 11218 (1990)