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首页> 外文期刊>Scientific reports. >Multivalley Free Energy Landscape and the Origin of Stripe and Quasi-Stripe CDW Structures in Monolayer MX2 Compounds
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Multivalley Free Energy Landscape and the Origin of Stripe and Quasi-Stripe CDW Structures in Monolayer MX2 Compounds

机译:Multivalley自由能景观与单层MX2化合物中条纹和准条纹CDW结构的起源

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Ultrathin sheets of transition metal dichalcogenides (MXsub2/sub) with charge density waves (CDWs) is increasingly gaining interest as a promising candidate for graphene-like devices. Although experimental data including stripe/quasi-stripe structure and hidden states have been reported, the ground state of ultrathin MXsub2/sub compounds and, in particular, the origin of anisotropic (stripe and quasi-stripe) CDW phases is a long-standing problem. Anisotropic CDW phases have been explained by Coulomb interaction between domain walls and inter-layer interaction. However, these models assume that anisotropic domain walls can exist in the first place. Here, we report that anisotropic CDW domain walls can appear naturally without assuming anisotropic interactions: We explain the origin of these phases by topological defect theory (line defects in a two-dimensional plane) and interference between harmonics of macroscopic CDW wave functions. We revisit the McMillan-Nakanishi-Shiba model for monolayer 1T-TaSsub2/sub and 2H-TaSesub2/sub and show that CDWs with wave vectors that are separated by 120° (i.e. the three-fold rotation symmetry of the underlying lattice) contain a free-energy landscape with many local minima. Then, we remove this 120° constraint and show that free energy local minima corresponding to the stripe and quasi-stripe phases appear. Our results imply that Coulomb interaction between domain walls and inter-layer interaction may be secondary factors for the appearance of stripe and quasi-stripe CDW phases. Furthermore, this model explains our recent experimental result (appearance of the quasi-stripe structure in monolayer 1T-TaSsub2/sub) and can predict new CDW phases, hence it may become the basis to study CDW further. We anticipate our results to be a starting point for further study in two-dimensional physics, such as explanation of "Hidden CDW states", study the interplay between supersolid symmetry and lattice symmetry, and application to other van der Waals structures.
机译:具有电荷密度波(CDW)的过渡金属二甲基甲基二巯基甲基二甲基α(MX 2 )越来越多地获得石墨烯装置的有希望的候选者。虽然已经报道了包括条纹/准条纹结构和隐藏状态的实验数据,但是超薄MX 2 化合物的地位,尤其是各向异性(条纹和准条带)CDW阶段的起源是一个长期存在的问题。通过畴壁和层间相互作用之间的库仑相互作用已经解释了各向异性CDW阶段。然而,这些模型假设各向异性畴壁可以首先存在。在这里,我们报告说,各向异性CDW畴壁可以自然出现而不假设各向异性相互作用:通过拓扑缺陷理论(二维平面中的线缺陷)解释这些阶段的起源,以及宏观CDW波函数的谐波之间的干扰。我们重新审视Monolayer 1T-Tas 2 和2h-Tase 2 的McMillan-Nakanishi-Shiba模型,并显示带有波动的CDW,其分隔120°(即底层格子的三倍旋转对称性含有许多局部最小值的自由能景观。然后,我们删除该120°约束,并显示对应于条纹和准条带相的自由能量局部最小值。我们的结果意味着畴壁和层间相互作用之间的库仑相互作用可能是条纹和准条纹CDW阶段外观的次要因素。此外,该模型解释了我们最近的实验结果(单层1T-Tas 2 的准条纹结构的外观,并且可以预测新的CDW阶段,因此可能成为进一步研究CDW的基础。我们预计我们的结果是在二维物理学中进一步研究的起点,例如解释“隐藏的CDW状态”,研究超负沙物对称性和晶格对称之间的相互作用,以及应用于其他范德瓦尔斯结构的应用。

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