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Effects of the Structure and Temperature on the Nature of Excitons in the Mo(0.6)W(0.4)S(2) Alloy

[Image: see text] We studied the nature of excitons in the transition metal dichalcogenide alloy Mo(0.6)W(0.4)S(2) compared to pure MoS(2) and WS(2) grown by atomic layer deposition (ALD). For this, optical absorption/transmission spectroscopy and time-dependent density functional theory (TDDFT) wer...

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Autores principales: Poonia, Deepika, Singh, Nisha, Schulpen, Jeff J. P. M., van der Laan, Marco, Maiti, Sourav, Failla, Michele, Kinge, Sachin, Bol, Ageeth A., Schall, Peter, Siebbeles, Laurens D. A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2022
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8819651/
https://www.ncbi.nlm.nih.gov/pubmed/35145573
http://dx.doi.org/10.1021/acs.jpcc.1c09806
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author Poonia, Deepika
Singh, Nisha
Schulpen, Jeff J. P. M.
van der Laan, Marco
Maiti, Sourav
Failla, Michele
Kinge, Sachin
Bol, Ageeth A.
Schall, Peter
Siebbeles, Laurens D. A.
author_facet Poonia, Deepika
Singh, Nisha
Schulpen, Jeff J. P. M.
van der Laan, Marco
Maiti, Sourav
Failla, Michele
Kinge, Sachin
Bol, Ageeth A.
Schall, Peter
Siebbeles, Laurens D. A.
author_sort Poonia, Deepika
collection PubMed
description [Image: see text] We studied the nature of excitons in the transition metal dichalcogenide alloy Mo(0.6)W(0.4)S(2) compared to pure MoS(2) and WS(2) grown by atomic layer deposition (ALD). For this, optical absorption/transmission spectroscopy and time-dependent density functional theory (TDDFT) were used. The effects of temperature on A and B exciton peak energies and line widths in optical transmission spectra were compared between the alloy and pure MoS(2) and WS(2). On increasing the temperature from 25 to 293 K, the energy of the A and B exciton peaks decreases, while their line width increases due to exciton–phonon interactions. The exciton–phonon interactions in the alloy are closer to those for MoS(2) than those for WS(2). This suggests that exciton wave functions in the alloy have a larger amplitude on Mo atoms than that on W atoms. The experimental absorption spectra could be reproduced by TDDFT calculations. Interestingly, for the alloy, the Mo and W atoms had to be distributed over all layers. Conversely, we could not reproduce the experimental alloy spectrum by calculations on a structure with alternating layers, in which every other layer contains only Mo atoms and the layers in between also contain W atoms. For the latter atomic arrangement, the TDDFT calculations yielded an additional optical absorption peak that could be due to excitons with some charge transfer character. From these results, we conclude that ALD yields an alloy in which Mo and W atoms are distributed uniformly among all layers.
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spelling pubmed-88196512022-02-08 Effects of the Structure and Temperature on the Nature of Excitons in the Mo(0.6)W(0.4)S(2) Alloy Poonia, Deepika Singh, Nisha Schulpen, Jeff J. P. M. van der Laan, Marco Maiti, Sourav Failla, Michele Kinge, Sachin Bol, Ageeth A. Schall, Peter Siebbeles, Laurens D. A. J Phys Chem C Nanomater Interfaces [Image: see text] We studied the nature of excitons in the transition metal dichalcogenide alloy Mo(0.6)W(0.4)S(2) compared to pure MoS(2) and WS(2) grown by atomic layer deposition (ALD). For this, optical absorption/transmission spectroscopy and time-dependent density functional theory (TDDFT) were used. The effects of temperature on A and B exciton peak energies and line widths in optical transmission spectra were compared between the alloy and pure MoS(2) and WS(2). On increasing the temperature from 25 to 293 K, the energy of the A and B exciton peaks decreases, while their line width increases due to exciton–phonon interactions. The exciton–phonon interactions in the alloy are closer to those for MoS(2) than those for WS(2). This suggests that exciton wave functions in the alloy have a larger amplitude on Mo atoms than that on W atoms. The experimental absorption spectra could be reproduced by TDDFT calculations. Interestingly, for the alloy, the Mo and W atoms had to be distributed over all layers. Conversely, we could not reproduce the experimental alloy spectrum by calculations on a structure with alternating layers, in which every other layer contains only Mo atoms and the layers in between also contain W atoms. For the latter atomic arrangement, the TDDFT calculations yielded an additional optical absorption peak that could be due to excitons with some charge transfer character. From these results, we conclude that ALD yields an alloy in which Mo and W atoms are distributed uniformly among all layers. American Chemical Society 2022-01-25 2022-02-03 /pmc/articles/PMC8819651/ /pubmed/35145573 http://dx.doi.org/10.1021/acs.jpcc.1c09806 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 Poonia, Deepika
Singh, Nisha
Schulpen, Jeff J. P. M.
van der Laan, Marco
Maiti, Sourav
Failla, Michele
Kinge, Sachin
Bol, Ageeth A.
Schall, Peter
Siebbeles, Laurens D. A.
Effects of the Structure and Temperature on the Nature of Excitons in the Mo(0.6)W(0.4)S(2) Alloy
title Effects of the Structure and Temperature on the Nature of Excitons in the Mo(0.6)W(0.4)S(2) Alloy
title_full Effects of the Structure and Temperature on the Nature of Excitons in the Mo(0.6)W(0.4)S(2) Alloy
title_fullStr Effects of the Structure and Temperature on the Nature of Excitons in the Mo(0.6)W(0.4)S(2) Alloy
title_full_unstemmed Effects of the Structure and Temperature on the Nature of Excitons in the Mo(0.6)W(0.4)S(2) Alloy
title_short Effects of the Structure and Temperature on the Nature of Excitons in the Mo(0.6)W(0.4)S(2) Alloy
title_sort effects of the structure and temperature on the nature of excitons in the mo(0.6)w(0.4)s(2) alloy
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8819651/
https://www.ncbi.nlm.nih.gov/pubmed/35145573
http://dx.doi.org/10.1021/acs.jpcc.1c09806
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