Emergent layer stacking arrangements in c-axis confined MoTe2

Abstract The layer stacking order in 2D materials strongly affects functional properties and holds promise for next-generation electronic devices. In bulk, octahedral MoTe2 possesses two stacking arrangements, the ferroelectric Weyl semimetal Td phase and the higher-order topological insulator 1T′ p...

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Main Authors: James L. Hart, Lopa Bhatt, Yanbing Zhu, Myung-Geun Han, Elisabeth Bianco, Shunran Li, David J. Hynek, John A. Schneeloch, Yu Tao, Despina Louca, Peijun Guo, Yimei Zhu, Felipe Jornada, Evan J. Reed, Lena F. Kourkoutis, Judy J. Cha
Format: Article
Language:English
Published: Nature Portfolio 2023-08-01
Series:Nature Communications
Online Access:https://doi.org/10.1038/s41467-023-40528-y
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author James L. Hart
Lopa Bhatt
Yanbing Zhu
Myung-Geun Han
Elisabeth Bianco
Shunran Li
David J. Hynek
John A. Schneeloch
Yu Tao
Despina Louca
Peijun Guo
Yimei Zhu
Felipe Jornada
Evan J. Reed
Lena F. Kourkoutis
Judy J. Cha
author_facet James L. Hart
Lopa Bhatt
Yanbing Zhu
Myung-Geun Han
Elisabeth Bianco
Shunran Li
David J. Hynek
John A. Schneeloch
Yu Tao
Despina Louca
Peijun Guo
Yimei Zhu
Felipe Jornada
Evan J. Reed
Lena F. Kourkoutis
Judy J. Cha
author_sort James L. Hart
collection DOAJ
description Abstract The layer stacking order in 2D materials strongly affects functional properties and holds promise for next-generation electronic devices. In bulk, octahedral MoTe2 possesses two stacking arrangements, the ferroelectric Weyl semimetal Td phase and the higher-order topological insulator 1T′ phase. However, in thin flakes of MoTe2, it is unclear if the layer stacking follows the Td, 1T′, or an alternative stacking sequence. Here, we use atomic-resolution scanning transmission electron microscopy to directly visualize the MoTe2 layer stacking. In thin flakes, we observe highly disordered stacking, with nanoscale 1T′ and Td domains, as well as alternative stacking arrangements not found in the bulk. We attribute these findings to intrinsic confinement effects on the MoTe2 stacking-dependent free energy. Our results are important for the understanding of exotic physics displayed in MoTe2 flakes. More broadly, this work suggests c-axis confinement as a method to influence layer stacking in other 2D materials.
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spelling doaj.art-90b58514477d4e1c81a49c6d74822f972023-11-20T09:59:08ZengNature PortfolioNature Communications2041-17232023-08-011411910.1038/s41467-023-40528-yEmergent layer stacking arrangements in c-axis confined MoTe2James L. Hart0Lopa Bhatt1Yanbing Zhu2Myung-Geun Han3Elisabeth Bianco4Shunran Li5David J. Hynek6John A. Schneeloch7Yu Tao8Despina Louca9Peijun Guo10Yimei Zhu11Felipe Jornada12Evan J. Reed13Lena F. Kourkoutis14Judy J. Cha15Department of Materials Science and Engineering, Cornell UniversitySchool of Applied and Engineering Physics, Cornell UniversityDepartment of Applied Physics, Stanford UniversityCondensed Matter Physics and Materials Science Department, Brookhaven National LaboratoryKavli Institute at Cornell for Nanoscale Science, Cornell UniversityDepartment of Chemical and Environmental Engineering, Yale UniversityEnergy Sciences Institute, Yale UniversityDepartment of Physics, University of VirginiaDepartment of Physics, University of VirginiaDepartment of Physics, University of VirginiaDepartment of Chemical and Environmental Engineering, Yale UniversityCondensed Matter Physics and Materials Science Department, Brookhaven National LaboratoryDepartment of Materials Science and Engineering, Stanford UniversityDepartment of Materials Science and Engineering, Stanford UniversitySchool of Applied and Engineering Physics, Cornell UniversityDepartment of Materials Science and Engineering, Cornell UniversityAbstract The layer stacking order in 2D materials strongly affects functional properties and holds promise for next-generation electronic devices. In bulk, octahedral MoTe2 possesses two stacking arrangements, the ferroelectric Weyl semimetal Td phase and the higher-order topological insulator 1T′ phase. However, in thin flakes of MoTe2, it is unclear if the layer stacking follows the Td, 1T′, or an alternative stacking sequence. Here, we use atomic-resolution scanning transmission electron microscopy to directly visualize the MoTe2 layer stacking. In thin flakes, we observe highly disordered stacking, with nanoscale 1T′ and Td domains, as well as alternative stacking arrangements not found in the bulk. We attribute these findings to intrinsic confinement effects on the MoTe2 stacking-dependent free energy. Our results are important for the understanding of exotic physics displayed in MoTe2 flakes. More broadly, this work suggests c-axis confinement as a method to influence layer stacking in other 2D materials.https://doi.org/10.1038/s41467-023-40528-y
spellingShingle James L. Hart
Lopa Bhatt
Yanbing Zhu
Myung-Geun Han
Elisabeth Bianco
Shunran Li
David J. Hynek
John A. Schneeloch
Yu Tao
Despina Louca
Peijun Guo
Yimei Zhu
Felipe Jornada
Evan J. Reed
Lena F. Kourkoutis
Judy J. Cha
Emergent layer stacking arrangements in c-axis confined MoTe2
Nature Communications
title Emergent layer stacking arrangements in c-axis confined MoTe2
title_full Emergent layer stacking arrangements in c-axis confined MoTe2
title_fullStr Emergent layer stacking arrangements in c-axis confined MoTe2
title_full_unstemmed Emergent layer stacking arrangements in c-axis confined MoTe2
title_short Emergent layer stacking arrangements in c-axis confined MoTe2
title_sort emergent layer stacking arrangements in c axis confined mote2
url https://doi.org/10.1038/s41467-023-40528-y
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