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Fine Structure Splitting of Phonon-Assisted Excitonic Transition in (PEA)(2)PbI(4) Two-Dimensional Perovskites

Two-dimensional van der Waals materials exhibit particularly strong excitonic effects, which causes them to be an exceptionally interesting platform for the investigation of exciton physics. A notable example is the two-dimensional Ruddlesden–Popper perovskites, where quantum and dielectric confinem...

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Autores principales: Posmyk, Katarzyna, Dyksik, Mateusz, Surrente, Alessandro, Zalewska, Katarzyna, Śmiertka, Maciej, Cybula, Ewelina, Paritmongkol, Watcharaphol, Tisdale, William A., Plochocka, Paulina, Baranowski, Michał
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10053047/
https://www.ncbi.nlm.nih.gov/pubmed/36986013
http://dx.doi.org/10.3390/nano13061119
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author Posmyk, Katarzyna
Dyksik, Mateusz
Surrente, Alessandro
Zalewska, Katarzyna
Śmiertka, Maciej
Cybula, Ewelina
Paritmongkol, Watcharaphol
Tisdale, William A.
Plochocka, Paulina
Baranowski, Michał
author_facet Posmyk, Katarzyna
Dyksik, Mateusz
Surrente, Alessandro
Zalewska, Katarzyna
Śmiertka, Maciej
Cybula, Ewelina
Paritmongkol, Watcharaphol
Tisdale, William A.
Plochocka, Paulina
Baranowski, Michał
author_sort Posmyk, Katarzyna
collection PubMed
description Two-dimensional van der Waals materials exhibit particularly strong excitonic effects, which causes them to be an exceptionally interesting platform for the investigation of exciton physics. A notable example is the two-dimensional Ruddlesden–Popper perovskites, where quantum and dielectric confinement together with soft, polar, and low symmetry lattice create a unique background for electron and hole interaction. Here, with the use of polarization-resolved optical spectroscopy, we have demonstrated that the simultaneous presence of tightly bound excitons, together with strong exciton–phonon coupling, allows for observing the exciton fine structure splitting of the phonon-assisted transitions of two-dimensional perovskite (PEA) [Formula: see text] PbI [Formula: see text] , where PEA stands for phenylethylammonium. We demonstrate that the phonon-assisted sidebands characteristic for (PEA) [Formula: see text] PbI [Formula: see text] are split and linearly polarized, mimicking the characteristics of the corresponding zero-phonon lines. Interestingly, the splitting of differently polarized phonon-assisted transitions can be different from that of the zero-phonon lines. We attribute this effect to the selective coupling of linearly polarized exciton states to non-degenerate phonon modes of different symmetries resulting from the low symmetry of (PEA) [Formula: see text] PbI [Formula: see text] lattice.
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spelling pubmed-100530472023-03-30 Fine Structure Splitting of Phonon-Assisted Excitonic Transition in (PEA)(2)PbI(4) Two-Dimensional Perovskites Posmyk, Katarzyna Dyksik, Mateusz Surrente, Alessandro Zalewska, Katarzyna Śmiertka, Maciej Cybula, Ewelina Paritmongkol, Watcharaphol Tisdale, William A. Plochocka, Paulina Baranowski, Michał Nanomaterials (Basel) Article Two-dimensional van der Waals materials exhibit particularly strong excitonic effects, which causes them to be an exceptionally interesting platform for the investigation of exciton physics. A notable example is the two-dimensional Ruddlesden–Popper perovskites, where quantum and dielectric confinement together with soft, polar, and low symmetry lattice create a unique background for electron and hole interaction. Here, with the use of polarization-resolved optical spectroscopy, we have demonstrated that the simultaneous presence of tightly bound excitons, together with strong exciton–phonon coupling, allows for observing the exciton fine structure splitting of the phonon-assisted transitions of two-dimensional perovskite (PEA) [Formula: see text] PbI [Formula: see text] , where PEA stands for phenylethylammonium. We demonstrate that the phonon-assisted sidebands characteristic for (PEA) [Formula: see text] PbI [Formula: see text] are split and linearly polarized, mimicking the characteristics of the corresponding zero-phonon lines. Interestingly, the splitting of differently polarized phonon-assisted transitions can be different from that of the zero-phonon lines. We attribute this effect to the selective coupling of linearly polarized exciton states to non-degenerate phonon modes of different symmetries resulting from the low symmetry of (PEA) [Formula: see text] PbI [Formula: see text] lattice. MDPI 2023-03-21 /pmc/articles/PMC10053047/ /pubmed/36986013 http://dx.doi.org/10.3390/nano13061119 Text en © 2023 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Posmyk, Katarzyna
Dyksik, Mateusz
Surrente, Alessandro
Zalewska, Katarzyna
Śmiertka, Maciej
Cybula, Ewelina
Paritmongkol, Watcharaphol
Tisdale, William A.
Plochocka, Paulina
Baranowski, Michał
Fine Structure Splitting of Phonon-Assisted Excitonic Transition in (PEA)(2)PbI(4) Two-Dimensional Perovskites
title Fine Structure Splitting of Phonon-Assisted Excitonic Transition in (PEA)(2)PbI(4) Two-Dimensional Perovskites
title_full Fine Structure Splitting of Phonon-Assisted Excitonic Transition in (PEA)(2)PbI(4) Two-Dimensional Perovskites
title_fullStr Fine Structure Splitting of Phonon-Assisted Excitonic Transition in (PEA)(2)PbI(4) Two-Dimensional Perovskites
title_full_unstemmed Fine Structure Splitting of Phonon-Assisted Excitonic Transition in (PEA)(2)PbI(4) Two-Dimensional Perovskites
title_short Fine Structure Splitting of Phonon-Assisted Excitonic Transition in (PEA)(2)PbI(4) Two-Dimensional Perovskites
title_sort fine structure splitting of phonon-assisted excitonic transition in (pea)(2)pbi(4) two-dimensional perovskites
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10053047/
https://www.ncbi.nlm.nih.gov/pubmed/36986013
http://dx.doi.org/10.3390/nano13061119
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