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激光冲击诱导单层石墨烯中的非对称三维弹塑性应变调制电子能量结构

Asymmetric 3D Elastic-Plastic Strain-Modulated Electron Energy Structure in Monolayer Graphene by Laser Shocking.

作者信息

Motlag Maithilee, Kumar Prashant, Hu Kevin Y, Jin Shengyu, Li Ji, Shao Jiayi, Yi Xuan, Lin Yen-Hsiang, Walrath Jenna C, Tong Lei, Huang Xinyu, Goldman Rachel S, Ye Lei, Cheng Gary J

机构信息

School of Industrial Engineering, Purdue University, West Lafayette, IN, 47907, USA.

Birck Nanotechnology Centre, Purdue University, West Lafayette, IN, 47907, USA.

出版信息

Adv Mater. 2019 May;31(19):e1900597. doi: 10.1002/adma.201900597. Epub 2019 Mar 29.

Abstract

Graphene has a great potential to replace silicon in prospective semiconductor industries due to its outstanding electronic and transport properties; nonetheless, its lack of energy bandgap is a substantial limitation for practical applications. To date, straining graphene to break its lattice symmetry is perhaps the most efficient approach toward realizing bandgap tunability in graphene. However, due to the weak lattice deformation induced by uniaxial or in-plane shear strain, most strained graphene studies have yielded bandgaps <1 eV. In this work, a modulated inhomogeneous local asymmetric elastic-plastic straining is reported that utilizes GPa-level laser shocking at a high strain rate (dε/dt) ≈ 10 -10 s , with excellent formability, inducing tunable bandgaps in graphene of up to 2.1 eV, as determined by scanning tunneling spectroscopy. High-resolution imaging and Raman spectroscopy reveal strain-induced modifications to the atomic and electronic structure in graphene and first-principles simulations predict the measured bandgap openings. Laser shock modulation of semimetallic graphene to a semiconducting material with controllable bandgap has the potential to benefit the electronic and optoelectronic industries.

摘要

由于其优异的电子和输运特性,石墨烯在未来的半导体产业中具有取代硅的巨大潜力;然而,其缺乏能带隙是实际应用中的一个重大限制。迄今为止,对石墨烯施加应变以打破其晶格对称性可能是实现石墨烯能带隙可调谐性的最有效方法。然而,由于单轴或面内剪切应变引起的晶格变形较弱,大多数应变石墨烯研究得到的能带隙小于1 eV。在这项工作中,报道了一种调制的非均匀局部非对称弹塑性应变,该应变利用GPa级激光在高应变速率(dε/dt)≈10⁹ s⁻¹下进行冲击,具有优异的可成形性,通过扫描隧道光谱法测定,在石墨烯中诱导出高达2.1 eV的可调谐能带隙。高分辨率成像和拉曼光谱揭示了应变引起的石墨烯原子和电子结构的变化,第一性原理模拟预测了测量到的能带隙开口。将半金属石墨烯激光冲击调制为具有可控能带隙的半导体材料,有望使电子和光电子产业受益。

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