Directional charge delocalization dynamics in semiconducting 2H-MoS $$_{2}$$ 2 and metallic 1T-Li $$_{\mathrm{x}}$$ x MoS $$_{2}$$ 2

Abstract The layered dichalcogenide MoS $$_{2}$$ 2 is relevant for electrochemical Li adsorption/intercalation, in the course of which the material undergoes a concomitant structural phase transition from semiconducting 2H-MoS $$_{2}$$ 2 to metallic 1T-Li $$_{\mathrm{x}}$$ x MoS $$_{2}$$ 2 . With th...

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Autores principales: Robert Haverkamp, Nomi L. A. N. Sorgenfrei, Erika Giangrisostomi, Stefan Neppl, Danilo Kühn, Alexander Föhlisch
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Publicado: Nature Portfolio 2021
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Acceso en línea:https://doaj.org/article/622e1a9ab82348c59f77e22d7c2fc629
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spelling oai:doaj.org-article:622e1a9ab82348c59f77e22d7c2fc6292021-12-02T16:35:56ZDirectional charge delocalization dynamics in semiconducting 2H-MoS $$_{2}$$ 2 and metallic 1T-Li $$_{\mathrm{x}}$$ x MoS $$_{2}$$ 210.1038/s41598-021-86364-22045-2322https://doaj.org/article/622e1a9ab82348c59f77e22d7c2fc6292021-03-01T00:00:00Zhttps://doi.org/10.1038/s41598-021-86364-2https://doaj.org/toc/2045-2322Abstract The layered dichalcogenide MoS $$_{2}$$ 2 is relevant for electrochemical Li adsorption/intercalation, in the course of which the material undergoes a concomitant structural phase transition from semiconducting 2H-MoS $$_{2}$$ 2 to metallic 1T-Li $$_{\mathrm{x}}$$ x MoS $$_{2}$$ 2 . With the core hole clock approach at the S L $$_{1}$$ 1 X-ray absorption edge we quantify the ultrafast directional charge transfer of excited S3p electrons in-plane ( $$\parallel$$ ‖ ) and out-of-plane ( $$\perp$$ ⊥ ) for 2H-MoS $$_{2}$$ 2 as $$\tau _{2H,\parallel } = 0.38 \pm 0.08$$ τ 2 H , ‖ = 0.38 ± 0.08 fs and $$\tau _{2H,\perp } = 0.33 \pm 0.06$$ τ 2 H , ⊥ = 0.33 ± 0.06 fs and for 1T-Li $$_{\mathrm{x}}$$ x MoS $$_{2}$$ 2 as $$\tau _{1T,\parallel } = 0.32 \pm 0.12$$ τ 1 T , ‖ = 0.32 ± 0.12 fs and $$\tau _{1T,\perp } = 0.09 \pm 0.07$$ τ 1 T , ⊥ = 0.09 ± 0.07 fs. The isotropic charge delocalization of S3p electrons in the semiconducting 2H phase within the S-Mo-S sheets is assigned to the specific symmetry of the Mo-S bonding arrangement. Formation of 1T-Li $$_{\mathrm{x}}$$ x MoS $$_{2}$$ 2 by lithiation accelerates the in-plane charge transfer by a factor of $$\sim 1.2$$ ∼ 1.2 due to electron injection to the Mo-S covalent bonds and concomitant structural repositioning of S atoms within the S-Mo-S sheets. For excitation into out-of-plane orbitals, an accelerated charge transfer by a factor of $$\sim 3.7$$ ∼ 3.7 upon lithiation occurs due to S-Li coupling.Robert HaverkampNomi L. A. N. SorgenfreiErika GiangrisostomiStefan NepplDanilo KühnAlexander FöhlischNature PortfolioarticleMedicineRScienceQENScientific Reports, Vol 11, Iss 1, Pp 1-7 (2021)
institution DOAJ
collection DOAJ
language EN
topic Medicine
R
Science
Q
spellingShingle Medicine
R
Science
Q
Robert Haverkamp
Nomi L. A. N. Sorgenfrei
Erika Giangrisostomi
Stefan Neppl
Danilo Kühn
Alexander Föhlisch
Directional charge delocalization dynamics in semiconducting 2H-MoS $$_{2}$$ 2 and metallic 1T-Li $$_{\mathrm{x}}$$ x MoS $$_{2}$$ 2
description Abstract The layered dichalcogenide MoS $$_{2}$$ 2 is relevant for electrochemical Li adsorption/intercalation, in the course of which the material undergoes a concomitant structural phase transition from semiconducting 2H-MoS $$_{2}$$ 2 to metallic 1T-Li $$_{\mathrm{x}}$$ x MoS $$_{2}$$ 2 . With the core hole clock approach at the S L $$_{1}$$ 1 X-ray absorption edge we quantify the ultrafast directional charge transfer of excited S3p electrons in-plane ( $$\parallel$$ ‖ ) and out-of-plane ( $$\perp$$ ⊥ ) for 2H-MoS $$_{2}$$ 2 as $$\tau _{2H,\parallel } = 0.38 \pm 0.08$$ τ 2 H , ‖ = 0.38 ± 0.08 fs and $$\tau _{2H,\perp } = 0.33 \pm 0.06$$ τ 2 H , ⊥ = 0.33 ± 0.06 fs and for 1T-Li $$_{\mathrm{x}}$$ x MoS $$_{2}$$ 2 as $$\tau _{1T,\parallel } = 0.32 \pm 0.12$$ τ 1 T , ‖ = 0.32 ± 0.12 fs and $$\tau _{1T,\perp } = 0.09 \pm 0.07$$ τ 1 T , ⊥ = 0.09 ± 0.07 fs. The isotropic charge delocalization of S3p electrons in the semiconducting 2H phase within the S-Mo-S sheets is assigned to the specific symmetry of the Mo-S bonding arrangement. Formation of 1T-Li $$_{\mathrm{x}}$$ x MoS $$_{2}$$ 2 by lithiation accelerates the in-plane charge transfer by a factor of $$\sim 1.2$$ ∼ 1.2 due to electron injection to the Mo-S covalent bonds and concomitant structural repositioning of S atoms within the S-Mo-S sheets. For excitation into out-of-plane orbitals, an accelerated charge transfer by a factor of $$\sim 3.7$$ ∼ 3.7 upon lithiation occurs due to S-Li coupling.
format article
author Robert Haverkamp
Nomi L. A. N. Sorgenfrei
Erika Giangrisostomi
Stefan Neppl
Danilo Kühn
Alexander Föhlisch
author_facet Robert Haverkamp
Nomi L. A. N. Sorgenfrei
Erika Giangrisostomi
Stefan Neppl
Danilo Kühn
Alexander Föhlisch
author_sort Robert Haverkamp
title Directional charge delocalization dynamics in semiconducting 2H-MoS $$_{2}$$ 2 and metallic 1T-Li $$_{\mathrm{x}}$$ x MoS $$_{2}$$ 2
title_short Directional charge delocalization dynamics in semiconducting 2H-MoS $$_{2}$$ 2 and metallic 1T-Li $$_{\mathrm{x}}$$ x MoS $$_{2}$$ 2
title_full Directional charge delocalization dynamics in semiconducting 2H-MoS $$_{2}$$ 2 and metallic 1T-Li $$_{\mathrm{x}}$$ x MoS $$_{2}$$ 2
title_fullStr Directional charge delocalization dynamics in semiconducting 2H-MoS $$_{2}$$ 2 and metallic 1T-Li $$_{\mathrm{x}}$$ x MoS $$_{2}$$ 2
title_full_unstemmed Directional charge delocalization dynamics in semiconducting 2H-MoS $$_{2}$$ 2 and metallic 1T-Li $$_{\mathrm{x}}$$ x MoS $$_{2}$$ 2
title_sort directional charge delocalization dynamics in semiconducting 2h-mos $$_{2}$$ 2 and metallic 1t-li $$_{\mathrm{x}}$$ x mos $$_{2}$$ 2
publisher Nature Portfolio
publishDate 2021
url https://doaj.org/article/622e1a9ab82348c59f77e22d7c2fc629
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