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化学气相沉积法生长的大面积石墨烯中声子等离激元的实空间成像。

Real-space imaging of acoustic plasmons in large-area graphene grown by chemical vapor deposition.

作者信息

Menabde Sergey G, Lee In-Ho, Lee Sanghyub, Ha Heonhak, Heiden Jacob T, Yoo Daehan, Kim Teun-Teun, Low Tony, Lee Young Hee, Oh Sang-Hyun, Jang Min Seok

机构信息

School of Electrical Engineering, Korea Advanced Institute of Science and Technology (KAIST), Daejeon, Korea.

Department of Electrical and Computer Engineering, University of Minnesota, Minneapolis, USA.

出版信息

Nat Commun. 2021 Feb 19;12(1):938. doi: 10.1038/s41467-021-21193-5.

DOI:10.1038/s41467-021-21193-5
PMID:33608541
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7895983/
Abstract

An acoustic plasmon mode in a graphene-dielectric-metal structure has recently been spotlighted as a superior platform for strong light-matter interaction. It originates from the coupling of graphene plasmon with its mirror image and exhibits the largest field confinement in the limit of a sub-nm-thick dielectric. Although recently detected in the far-field regime, optical near-fields of this mode are yet to be observed and characterized. Here, we demonstrate a direct optical probing of the plasmonic fields reflected by the edges of graphene via near-field scattering microscope, revealing a relatively small propagation loss of the mid-infrared acoustic plasmons in our devices that allows for their real-space mapping at ambient conditions even with unprotected, large-area graphene grown by chemical vapor deposition. We show an acoustic plasmon mode that is twice as confined and has 1.4 times higher figure of merit in terms of the normalized propagation length compared to the graphene surface plasmon under similar conditions. We also investigate the behavior of the acoustic graphene plasmons in a periodic array of gold nanoribbons. Our results highlight the promise of acoustic plasmons for graphene-based optoelectronics and sensing applications.

摘要

最近,石墨烯 - 电介质 - 金属结构中的声学等离子体激元模式作为强光 - 物质相互作用的卓越平台受到了关注。它源于石墨烯等离子体激元与其镜像的耦合,并且在亚纳米厚电介质极限下表现出最大的场限制。尽管最近在远场区域被检测到,但这种模式的光学近场尚未被观察和表征。在这里,我们通过近场散射显微镜展示了对石墨烯边缘反射的等离子体激元场的直接光学探测,揭示了我们器件中中红外声学等离子体激元相对较小的传播损耗,这使得即使在环境条件下,对于通过化学气相沉积生长的未受保护的大面积石墨烯,也能够对其进行实空间映射。我们展示了一种声学等离子体激元模式,与类似条件下的石墨烯表面等离子体激元相比,其限制程度高出两倍,并且在归一化传播长度方面的品质因数高1.4倍。我们还研究了金纳米带周期性阵列中声学石墨烯等离子体激元的行为。我们的结果突出了声学等离子体激元在基于石墨烯的光电子学和传感应用中的前景。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/11dd/7895983/19c990b8c837/41467_2021_21193_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/11dd/7895983/cdc530a9d9d5/41467_2021_21193_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/11dd/7895983/4b3d12c6dfdd/41467_2021_21193_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/11dd/7895983/2bde1dcaa94e/41467_2021_21193_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/11dd/7895983/14d5b9cc0eb1/41467_2021_21193_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/11dd/7895983/19c990b8c837/41467_2021_21193_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/11dd/7895983/cdc530a9d9d5/41467_2021_21193_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/11dd/7895983/4b3d12c6dfdd/41467_2021_21193_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/11dd/7895983/2bde1dcaa94e/41467_2021_21193_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/11dd/7895983/14d5b9cc0eb1/41467_2021_21193_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/11dd/7895983/19c990b8c837/41467_2021_21193_Fig5_HTML.jpg

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