Li Wenhua, Tian Wenchao
School of Electro-Mechanical Engineering, Xidian University, Xi'an 710071, China.
Nanomaterials (Basel). 2022 May 18;12(10):1722. doi: 10.3390/nano12101722.
Due to the limitation of graphene processing technology, the prepared graphene inevitably contains various defects. The defects will have a particular influence on the macroscopic characteristics of the graphene. In this paper, the defect-based graphene nanoresonators are studied. In this study, the resonant properties of graphene were investigated via molecular dynamic simulations. The effect of vacancy defects and hole defects at different positions, numbers, and concentrations on the resonance frequency of graphene nanoribbons was studied. The results indicated that single monatomic vacancy has no effect on graphene resonant frequency, and the concentration of the resonant frequency of graphene decreases almost linearly with the increase of single-atom vacancy concentration. When the vacancy concentration is 5%, the resonance frequency is reduced by 12.77% compared to the perfect graphene. Holes on the graphene cause the resonance frequency to decrease. As the circular hole defect is closer to the center of the graphene nanoribbon, not only does its resonant frequency increase, but the tuning range is also expanded accordingly. Under the external force of 10.715 nN, the resonant frequency of graphene reaches 429.57 GHz when the circular hole is located at the center of the graphene nanoribbon, which is 40 GHz lower than that of single vacancy defect graphene. When the circular hole is close to the fixed end of graphene, the resonant frequency is 379.62 GHz, which is 90 GHz lower than that of single vacancy graphene. When the hole defect is at the center of nanoribbon, the frequency tunable range of graphene reaches 120 GHz. The tunable frequency range of graphene is 100.12 GHz when the hole defect is near the fixed ends of the graphene nanoribbon. This work is of great significance for design and performance optimization of graphene-based nanoelectro-mechanical system (NEMS) resonators.
由于石墨烯加工技术的限制,制备出的石墨烯不可避免地含有各种缺陷。这些缺陷会对石墨烯的宏观特性产生特定影响。本文对基于缺陷的石墨烯纳米谐振器进行了研究。在本研究中,通过分子动力学模拟研究了石墨烯的谐振特性。研究了不同位置、数量和浓度的空位缺陷和孔洞缺陷对石墨烯纳米带谐振频率的影响。结果表明,单个单原子空位对石墨烯谐振频率没有影响,且石墨烯谐振频率的浓度几乎随单原子空位浓度的增加呈线性下降。当空位浓度为5%时,与完美石墨烯相比,谐振频率降低了12.77%。石墨烯上的孔洞会导致谐振频率降低。随着圆形孔洞缺陷离石墨烯纳米带中心越近,其谐振频率不仅增加,而且调谐范围也相应扩大。在10.715 nN的外力作用下,当圆形孔洞位于石墨烯纳米带中心时,石墨烯的谐振频率达到429.57 GHz,比单空位缺陷石墨烯低40 GHz。当圆形孔洞靠近石墨烯固定端时,谐振频率为379.62 GHz,比单空位石墨烯低90 GHz。当孔洞缺陷位于纳米带中心时,石墨烯的频率可调范围达到120 GHz。当孔洞缺陷靠近石墨烯纳米带固定端时,石墨烯的可调频率范围为100.12 GHz。这项工作对基于石墨烯的纳米机电系统(NEMS)谐振器的设计和性能优化具有重要意义。