区分使用化学气相沉积法生长的 WSe2 双层膜中的不同叠层

Aymen Mahmoudi, Meryem Bouaziz, Davide Romani, Marco Pala, Aurelien Thieffry, Thibault Brule, Julien Chaste, Fabrice Oehler, Abdelkarim Ouerghi
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引用次数: 0

摘要

二维过渡金属二掺杂物(TMDs)的堆积顺序作为范德华超结构的重要组成部分,正引起人们的极大兴趣。区分 AAprime(2H)和 AB(3R)构型的常用快速方法是利用光学图像中每个三角形层的相对边缘取向(theta)。在这里,我们要强调的是,仅凭这种方法还不足以完全确定堆叠顺序。相反,我们提出了一种利用二次谐波发生(SHG)和拉曼斯谱精确确定 WSe2 双层构型的模型和方法。我们证明 AB 相(theta = 0)deg 层的 SHG 响应比单层结构的信号更强。然而,在同双层 WSe2 的 AAprime 相和 ABprime 相(theta = 60deg 和 0deg 分别)中,SHG 完全消失。此外,研究还发现同双层 WSe2 的一些光学特性取决于堆叠顺序的细节,其中低频(LF)拉曼频率的差异最为明显,这一点已得到 DFT 模拟的证实。这样就可以对 TMD 中的堆积顺序进行明确、高通量、非破坏性的识别,而这一新兴研究领域还没有有力地解决这一问题。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Distinguishing different stackings in WSe2 bilayers grown Using Chemical Vapor Deposition
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.
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