Despite its simple crystal structure, layered boron nitride features a surprisingly complex variety of phonon-assisted luminescence peaks. We present a combined experimental and theoretical study on ultraviolet-light emission in hexagonal and rhombohedral bulk boron nitride crystals. Emission spectra of high-quality samples are measured via cathodoluminescence spectroscopy, displaying characteristic differences between the two polytypes. These differences are explained using a fully first-principles computational technique that takes into account radiative emission from "indirect," finite-momentum excitons via coupling to finite-momentum phonons. We show that the differences in peak positions, number of peaks, and relative intensities can be qualitatively and quantitatively explained, once a full integration over all relevant momenta of excitons and phonons is performed.
Distinguishing Different Stackings in Layered Materials via Luminescence Spectroscopy / Zanfrognini, M.; Plaud, A.; Stenger, I.; Fossard, F.; Sponza, L.; Schue, L.; Paleari, F.; Molinari, E.; Varsano, D.; Wirtz, L.; Ducastelle, F.; Loiseau, A.; Barjon, J.. - In: PHYSICAL REVIEW LETTERS. - ISSN 1079-7114. - 131:20(2023), pp. 206902-206902. [10.1103/PhysRevLett.131.206902]
Distinguishing Different Stackings in Layered Materials via Luminescence Spectroscopy
Zanfrognini M.;Molinari E.;
2023
Abstract
Despite its simple crystal structure, layered boron nitride features a surprisingly complex variety of phonon-assisted luminescence peaks. We present a combined experimental and theoretical study on ultraviolet-light emission in hexagonal and rhombohedral bulk boron nitride crystals. Emission spectra of high-quality samples are measured via cathodoluminescence spectroscopy, displaying characteristic differences between the two polytypes. These differences are explained using a fully first-principles computational technique that takes into account radiative emission from "indirect," finite-momentum excitons via coupling to finite-momentum phonons. We show that the differences in peak positions, number of peaks, and relative intensities can be qualitatively and quantitatively explained, once a full integration over all relevant momenta of excitons and phonons is performed.File | Dimensione | Formato | |
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