Tunable Electronic Properties of Lateral Monolayer Transition Metal Dichalcogenide Superlattice Nanoribbons

The structural stability and structural and electronic properties of lateral monolayer transition metal chalcogenide superlattice zigzag and armchair nanoribbons have been studied by employing a first-principles method based on the density functional theory. The main focus is to study the effects of...

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Main Authors: Jinhua Wang, Gyaneshwar P. Srivastava
Format: Article
Language:English
Published: MDPI AG 2021-02-01
Series:Nanomaterials
Subjects:
Online Access:https://www.mdpi.com/2079-4991/11/2/534
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spelling doaj-db85214abb15490bb513593a4ce8f77f2021-02-20T00:05:47ZengMDPI AGNanomaterials2079-49912021-02-011153453410.3390/nano11020534Tunable Electronic Properties of Lateral Monolayer Transition Metal Dichalcogenide Superlattice NanoribbonsJinhua Wang0Gyaneshwar P. Srivastava1School of Science, Tianjin University of Technology and Education, Tianjin 300222, ChinaSchool of Physics, University of Exeter, Exeter EX4 4QL, UKThe structural stability and structural and electronic properties of lateral monolayer transition metal chalcogenide superlattice zigzag and armchair nanoribbons have been studied by employing a first-principles method based on the density functional theory. The main focus is to study the effects of varying the width and periodicity of nanoribbon, varying cationic and anionic elements of superlattice parent compounds, biaxial strain, and nanoribbon edge passivation with different elements. The band gap opens up when the (MoS<sub>2</sub>)<sub>3</sub>/(WS<sub>2</sub>)<sub>3</sub> and (MoS<sub>2</sub>)<sub>3</sub>/(MoTe<sub>2</sub>)<sub>3</sub> armchair nanoribbons are passivated by H, S and O atoms. The H and O co-passivated (MoS<sub>2</sub>)<sub>3</sub>/(WS<sub>2</sub>)<sub>3</sub> armchair nanoribbon exhibits higher energy band gap. The band gap with the edge S vacancy connecting to the W atom is much smaller than the S vacancy connecting to the Mo atom. Small band gaps are obtained for both edge and inside Mo vacancies. There is a clear difference in the band gap states between inside and edge Mo vacancies for symmetric nanoribbon structure, while there is only a slight difference for asymmetric structure. The electronic orbitals of atoms around Mo vacancy play an important role in determining the valence band maximum, conduction band minimum, and impurity level in the band gap.https://www.mdpi.com/2079-4991/11/2/534electronic propertiesfirst-principleedge passivationvacancybiaxial strain
collection DOAJ
language English
format Article
sources DOAJ
author Jinhua Wang
Gyaneshwar P. Srivastava
spellingShingle Jinhua Wang
Gyaneshwar P. Srivastava
Tunable Electronic Properties of Lateral Monolayer Transition Metal Dichalcogenide Superlattice Nanoribbons
Nanomaterials
electronic properties
first-principle
edge passivation
vacancy
biaxial strain
author_facet Jinhua Wang
Gyaneshwar P. Srivastava
author_sort Jinhua Wang
title Tunable Electronic Properties of Lateral Monolayer Transition Metal Dichalcogenide Superlattice Nanoribbons
title_short Tunable Electronic Properties of Lateral Monolayer Transition Metal Dichalcogenide Superlattice Nanoribbons
title_full Tunable Electronic Properties of Lateral Monolayer Transition Metal Dichalcogenide Superlattice Nanoribbons
title_fullStr Tunable Electronic Properties of Lateral Monolayer Transition Metal Dichalcogenide Superlattice Nanoribbons
title_full_unstemmed Tunable Electronic Properties of Lateral Monolayer Transition Metal Dichalcogenide Superlattice Nanoribbons
title_sort tunable electronic properties of lateral monolayer transition metal dichalcogenide superlattice nanoribbons
publisher MDPI AG
series Nanomaterials
issn 2079-4991
publishDate 2021-02-01
description The structural stability and structural and electronic properties of lateral monolayer transition metal chalcogenide superlattice zigzag and armchair nanoribbons have been studied by employing a first-principles method based on the density functional theory. The main focus is to study the effects of varying the width and periodicity of nanoribbon, varying cationic and anionic elements of superlattice parent compounds, biaxial strain, and nanoribbon edge passivation with different elements. The band gap opens up when the (MoS<sub>2</sub>)<sub>3</sub>/(WS<sub>2</sub>)<sub>3</sub> and (MoS<sub>2</sub>)<sub>3</sub>/(MoTe<sub>2</sub>)<sub>3</sub> armchair nanoribbons are passivated by H, S and O atoms. The H and O co-passivated (MoS<sub>2</sub>)<sub>3</sub>/(WS<sub>2</sub>)<sub>3</sub> armchair nanoribbon exhibits higher energy band gap. The band gap with the edge S vacancy connecting to the W atom is much smaller than the S vacancy connecting to the Mo atom. Small band gaps are obtained for both edge and inside Mo vacancies. There is a clear difference in the band gap states between inside and edge Mo vacancies for symmetric nanoribbon structure, while there is only a slight difference for asymmetric structure. The electronic orbitals of atoms around Mo vacancy play an important role in determining the valence band maximum, conduction band minimum, and impurity level in the band gap.
topic electronic properties
first-principle
edge passivation
vacancy
biaxial strain
url https://www.mdpi.com/2079-4991/11/2/534
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AT gyaneshwarpsrivastava tunableelectronicpropertiesoflateralmonolayertransitionmetaldichalcogenidesuperlatticenanoribbons
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