Department of Physics , North Carolina State University , Raleigh , North Carolina 27695 , United States.
Department of Materials Science and Engineering , North Carolina State University , Raleigh , North Carolina 27695 , United States.
Nano Lett. 2019 Feb 13;19(2):1104-1111. doi: 10.1021/acs.nanolett.8b04408. Epub 2019 Jan 14.
Many-body interactions in photoexcited semiconductors can bring about strongly interacting electronic states, culminating in the fully ionized matter of electron-hole plasma (EHP) and electron-hole liquid (EHL). These exotic phases exhibit unique electronic properties, such as metallic conductivity and metastable high photoexcitation density, which can be the basis for future transformative applications. However, the cryogenic condition required for its formation has limited the study of dense plasma phases to a purely academic pursuit in a restricted parameter space. This paradigm can potentially change with the recent experimental observation of these phases in atomically thin MoS and MoTe at room temperature. A fundamental understanding of EHP and EHL dynamics is critical for developing novel applications on this versatile layered platform. In this work, we studied the formation and dissipation of EHP in monolayer MoS. Unlike previous results in bulk semiconductors, our results reveal that electromechanical material changes in monolayer MoS during photoexcitation play a significant role in dense EHP formation. Within the free-standing geometry, photoexcitation is accompanied by an unconstrained thermal expansion, resulting in a direct-to-indirect gap electronic transition at a critical lattice spacing and fluence. This dramatic altering of the material's energetic landscape extends carrier lifetimes by 2 orders of magnitude and allows the density required for EHP formation. The result is a stable dense plasma state that is sustained with modest optical photoexcitation. Our findings pave the way for novel applications based on dense plasma states in two-dimensional semiconductors.
多体相互作用在光激发半导体中可以产生强相互作用的电子态,最终导致电子-空穴等离子体(EHP)和电子-空穴液体(EHL)的完全离化物质。这些奇特的相具有独特的电子特性,如金属导电性和亚稳态的高光激发密度,这可以为未来的变革性应用提供基础。然而,其形成所需的低温条件限制了对高密度等离子体相的研究仅限于在有限的参数空间内进行纯学术探讨。这种范式可能会随着最近在室温下原子层厚的 MoS 和 MoTe 中观察到这些相而发生改变。对 EHP 和 EHL 动力学的基本理解对于在这个多功能的层状平台上开发新的应用至关重要。在这项工作中,我们研究了单层 MoS 中 EHP 的形成和耗散。与体半导体中的先前结果不同,我们的结果表明,单层 MoS 中光激发时的机电材料变化在高密度 EHP 形成中起着重要作用。在自由支撑的几何形状中,光激发伴随着不受约束的热膨胀,导致在临界晶格间距和光通量下发生直接到间接带隙的电子跃迁。这种材料能态的剧烈改变将载流子寿命延长了 2 个数量级,并允许形成 EHP 所需的密度。结果是形成了一种稳定的高密度等离子体状态,可以通过适度的光激发来维持。我们的发现为基于二维半导体中的高密度等离子体状态的新型应用铺平了道路。