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有自由边缘和无自由边缘的石墨烯机械谐振器中的能量耗散

Energy Dissipation in Graphene Mechanical Resonators with and without Free Edges.

作者信息

Takamura Makoto, Okamoto Hajime, Furukawa Kazuaki, Yamaguchi Hiroshi, Hibino Hiroki

机构信息

NTT Basic Research Laboratories, NTT Corporation, 3-1 Morinosato Wakamiya, Atsugi, Kanagawa 243-0198, Japan.

出版信息

Micromachines (Basel). 2016 Sep 5;7(9):158. doi: 10.3390/mi7090158.

DOI:10.3390/mi7090158
PMID:30404329
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6190471/
Abstract

Graphene-based nanoelectromechanical systems (NEMS) have high future potential to realize sensitive mass and force sensors owing to graphene's low mass density and exceptional mechanical properties. One of the important remaining issues in this field is how to achieve mechanical resonators with a high quality factor (). Energy dissipation in resonators decreases , and suppressing it is the key to realizing sensitive sensors. In this article, we review our recent work on energy dissipation in doubly-clamped and circular drumhead graphene resonators. We examined the temperature () dependence of the inverse of a quality factor ( Q - 1 ) to reveal what the dominant dissipation mechanism is. Our doubly-clamped trilayer resonators show a characteristic Q - 1 - curve similar to that observed in monolayer resonators: Q - 1 ∝ T 2 above ∼100 K and ∝ T 0.3 below ∼100 K. By comparing our results with previous experimental and theoretical results, we determine that the T 2 and T 0.3 dependences can be attributed to tensile strain induced by clamping metals and vibrations at the free edges in doubly-clamped resonators, respectively. The Q - 1 - curve in our circular drumhead resonators indicates that removing free edges and clamping metal suppresses energy dissipation in the resonators, resulting in a linear dependence of Q - 1 in a wide temperature range.

摘要

基于石墨烯的纳米机电系统(NEMS)因其低质量密度和出色的机械性能,在实现灵敏的质量和力传感器方面具有很高的未来潜力。该领域仍存在的一个重要问题是如何实现具有高品质因数( )的机械谐振器。谐振器中的能量耗散会降低 ,抑制能量耗散是实现灵敏传感器的关键。在本文中,我们回顾了我们最近在双端固定和圆形鼓面石墨烯谐振器能量耗散方面的工作。我们研究了品质因数倒数(Q - 1)对温度( )的依赖性,以揭示主要的耗散机制是什么。我们的双端固定三层谐振器显示出与单层谐振器中观察到的类似的特征Q - 1曲线:在约100 K以上,Q - 1 ∝ T 2,在约100 K以下,Q - 1 ∝ T 0.3。通过将我们的结果与先前的实验和理论结果进行比较,我们确定T 2和T 0.3依赖性分别可归因于双端固定谐振器中夹紧金属引起的拉伸应变和自由边缘处的振动。我们圆形鼓面谐振器中的Q - 1曲线表明,去除自由边缘和夹紧金属可抑制谐振器中的能量耗散,从而在很宽的温度范围内导致Q - 1呈线性 依赖性。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4f40/6190471/c0a423b9173a/micromachines-07-00158-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4f40/6190471/a05b4245e52d/micromachines-07-00158-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4f40/6190471/1d6761c73105/micromachines-07-00158-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4f40/6190471/5a64f2df88d4/micromachines-07-00158-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4f40/6190471/f673c1135dbe/micromachines-07-00158-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4f40/6190471/5c13e096722c/micromachines-07-00158-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4f40/6190471/f4aba9f31b2b/micromachines-07-00158-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4f40/6190471/c0a423b9173a/micromachines-07-00158-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4f40/6190471/a05b4245e52d/micromachines-07-00158-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4f40/6190471/1d6761c73105/micromachines-07-00158-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4f40/6190471/5a64f2df88d4/micromachines-07-00158-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4f40/6190471/f673c1135dbe/micromachines-07-00158-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4f40/6190471/5c13e096722c/micromachines-07-00158-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4f40/6190471/f4aba9f31b2b/micromachines-07-00158-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4f40/6190471/c0a423b9173a/micromachines-07-00158-g007.jpg

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Observation of decoherence in a carbon nanotube mechanical resonator.观察碳纳米管机械谐振器中的退相干现象。
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