{"title":"Distinguishing different stackings in WSe2 bilayers grown Using Chemical Vapor Deposition","authors":"Aymen Mahmoudi, Meryem Bouaziz, Davide Romani, Marco Pala, Aurelien Thieffry, Thibault Brule, Julien Chaste, Fabrice Oehler, Abdelkarim Ouerghi","doi":"arxiv-2409.08617","DOIUrl":null,"url":null,"abstract":"The stacking order of two-dimensional transition metal dichalcogenides (TMDs)\nis attracting tremendous interest as an essential component of van der Waals\nheterostructures. A common and fast approach to distinguish between the AAprime\n(2H) and AB (3R) configurations uses the relative edge orientation of each\ntriangular layer (theta) from optical images. Here, we highlight that this\nmethod alone is not sufficient to fully identify the stacking order. Instead we\npropose a model and methodology to accurately determine the bilayer\nconfiguration of WSe2 using second harmonic generation (SHG) and Raman\nspectroscopy. We demonstrate that the SHG response of the AB phase (theta = 0)\ndeg layers is more intense than the signal from the single layer structure.\nHowever, the SHG totally vanishes in the AAprime and ABprime phases (theta = 60\ndeg) and 0 deg respectively) of homo-bilayer WSe2. Also, several optical\nfeatures of homo-bilayer WSe2 are found to depend on the details of the\nstacking order, with the difference being the clearest in the low frequency\n(LF) Raman frequencies, as confirmed by DFT simulation. This allows\nunambiguous, high-throughput, nondestructive identification of stacking order\nin TMDs, which is not robustly addressed in this emerging research area.","PeriodicalId":501137,"journal":{"name":"arXiv - PHYS - Mesoscale and Nanoscale Physics","volume":"10 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Mesoscale and Nanoscale Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.08617","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
The stacking order of two-dimensional transition metal dichalcogenides (TMDs)
is attracting tremendous interest as an essential component of van der Waals
heterostructures. A common and fast approach to distinguish between the AAprime
(2H) and AB (3R) configurations uses the relative edge orientation of each
triangular layer (theta) from optical images. Here, we highlight that this
method alone is not sufficient to fully identify the stacking order. Instead we
propose a model and methodology to accurately determine the bilayer
configuration of WSe2 using second harmonic generation (SHG) and Raman
spectroscopy. We demonstrate that the SHG response of the AB phase (theta = 0)
deg layers is more intense than the signal from the single layer structure.
However, the SHG totally vanishes in the AAprime and ABprime phases (theta = 60
deg) and 0 deg respectively) of homo-bilayer WSe2. Also, several optical
features of homo-bilayer WSe2 are found to depend on the details of the
stacking order, with the difference being the clearest in the low frequency
(LF) Raman frequencies, as confirmed by DFT simulation. This allows
unambiguous, high-throughput, nondestructive identification of stacking order
in TMDs, which is not robustly addressed in this emerging research area.