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“Dead” Exciton Layer and Exciton Anisotropy of Bulk MoS(2) Extracted from Optical Measurements

[Image: see text] Excitons (electron–hole pairs bound by the Coulomb potential) play an important role in optical and electronic properties of layered materials. They can be used to modulate light with high frequencies due to the optical Pauli blocking. The properties of excitons in 2D materials are...

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Autores principales: Kravets, Vasyl G., Zhukov, Alexander A., Holwill, Matthew, Novoselov, Kostya S., Grigorenko, Alexander N.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2022
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9706669/
https://www.ncbi.nlm.nih.gov/pubmed/36351038
http://dx.doi.org/10.1021/acsnano.2c07169
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author Kravets, Vasyl G.
Zhukov, Alexander A.
Holwill, Matthew
Novoselov, Kostya S.
Grigorenko, Alexander N.
author_facet Kravets, Vasyl G.
Zhukov, Alexander A.
Holwill, Matthew
Novoselov, Kostya S.
Grigorenko, Alexander N.
author_sort Kravets, Vasyl G.
collection PubMed
description [Image: see text] Excitons (electron–hole pairs bound by the Coulomb potential) play an important role in optical and electronic properties of layered materials. They can be used to modulate light with high frequencies due to the optical Pauli blocking. The properties of excitons in 2D materials are extremely anisotropic. However, due to nanometre sizes of excitons and their short life times, reliable tools to study this anisotropy are lacking. Here, we show how direct optical reflection measurements can be used to evaluate anisotropy of excitons in transition metal dichalcogenides MoS(2). Using focused beam spectroscopic ellipsometry, we have measured the polarized optical reflection of bulk MoS(2) for two crystal orientations: c-axis being perpendicular to the surface from which reflection is measured and c-axis being parallel to the surface from which reflection is measured. We found that for the parallel configuration the optical reflection near excitonic transitions is strongly affected by the presence of the exciton “dead” layer such that the excitonic reflection peaks become the excitonic dips due to light interference. At the same time, the optical reflection for the perpendicular orientation is not significantly altered by the exciton “dead” layer due to large anisotropy of exciton properties. Performing simultaneous Fresnel fitting for both geometries, we were able to evaluate exciton anisotropy in layered materials from simple optical measurements.
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spelling pubmed-97066692022-11-30 “Dead” Exciton Layer and Exciton Anisotropy of Bulk MoS(2) Extracted from Optical Measurements Kravets, Vasyl G. Zhukov, Alexander A. Holwill, Matthew Novoselov, Kostya S. Grigorenko, Alexander N. ACS Nano [Image: see text] Excitons (electron–hole pairs bound by the Coulomb potential) play an important role in optical and electronic properties of layered materials. They can be used to modulate light with high frequencies due to the optical Pauli blocking. The properties of excitons in 2D materials are extremely anisotropic. However, due to nanometre sizes of excitons and their short life times, reliable tools to study this anisotropy are lacking. Here, we show how direct optical reflection measurements can be used to evaluate anisotropy of excitons in transition metal dichalcogenides MoS(2). Using focused beam spectroscopic ellipsometry, we have measured the polarized optical reflection of bulk MoS(2) for two crystal orientations: c-axis being perpendicular to the surface from which reflection is measured and c-axis being parallel to the surface from which reflection is measured. We found that for the parallel configuration the optical reflection near excitonic transitions is strongly affected by the presence of the exciton “dead” layer such that the excitonic reflection peaks become the excitonic dips due to light interference. At the same time, the optical reflection for the perpendicular orientation is not significantly altered by the exciton “dead” layer due to large anisotropy of exciton properties. Performing simultaneous Fresnel fitting for both geometries, we were able to evaluate exciton anisotropy in layered materials from simple optical measurements. American Chemical Society 2022-11-09 2022-11-22 /pmc/articles/PMC9706669/ /pubmed/36351038 http://dx.doi.org/10.1021/acsnano.2c07169 Text en © 2022 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by/4.0/Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Kravets, Vasyl G.
Zhukov, Alexander A.
Holwill, Matthew
Novoselov, Kostya S.
Grigorenko, Alexander N.
“Dead” Exciton Layer and Exciton Anisotropy of Bulk MoS(2) Extracted from Optical Measurements
title “Dead” Exciton Layer and Exciton Anisotropy of Bulk MoS(2) Extracted from Optical Measurements
title_full “Dead” Exciton Layer and Exciton Anisotropy of Bulk MoS(2) Extracted from Optical Measurements
title_fullStr “Dead” Exciton Layer and Exciton Anisotropy of Bulk MoS(2) Extracted from Optical Measurements
title_full_unstemmed “Dead” Exciton Layer and Exciton Anisotropy of Bulk MoS(2) Extracted from Optical Measurements
title_short “Dead” Exciton Layer and Exciton Anisotropy of Bulk MoS(2) Extracted from Optical Measurements
title_sort “dead” exciton layer and exciton anisotropy of bulk mos(2) extracted from optical measurements
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9706669/
https://www.ncbi.nlm.nih.gov/pubmed/36351038
http://dx.doi.org/10.1021/acsnano.2c07169
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