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通过凯库勒-奥工程实现石墨烯中的原子级薄电流路径。

Atomically Thin Current Pathways in Graphene through Kekulé-O Engineering.

作者信息

García Santiago Galván Y, Betancur-Ocampo Yonatan, Sánchez-Ochoa Francisco, Stegmann Thomas

机构信息

Instituto de Ciencias Físicas, Universidad Nacional Autónoma de México, 62210 Cuernavaca, México.

Instituto de Física, Universidad Nacional Autónoma de México, 04510 Ciudad de México, México.

出版信息

Nano Lett. 2024 Feb 21;24(7):2322-2327. doi: 10.1021/acs.nanolett.3c04703. Epub 2024 Feb 8.

DOI:10.1021/acs.nanolett.3c04703
PMID:38329068
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10885192/
Abstract

We demonstrate that the current flow in graphene can be guided on atomically thin current pathways by the engineering of Kekulé-O distortions. A grain boundary in these distortions separates the system into topologically distinct regions and induces a ballistic domain-wall state. The state is independent of the orientation of the grain boundary with respect to the graphene sublattice and permits guiding the current on arbitrary paths. As the state is gapped, the current flow can be switched by electrostatic gates. Our findings are explained by a generalization of the Jackiw-Rebbi model, where the electrons behave in one region of the system as Fermions with an effective complex mass, making the device not only promising for technological applications but also a test-ground for concepts from high-energy physics. An atomic model supported by DFT calculations demonstrates that the system can be realized by decorating graphene with Ti atoms.

摘要

我们证明,通过对凯库勒 - O 畸变进行工程设计,石墨烯中的电流可以在原子级薄的电流路径上被引导。这些畸变中的晶界将系统分隔成拓扑上不同的区域,并诱导出弹道畴壁态。该状态与晶界相对于石墨烯子晶格的取向无关,并允许电流在任意路径上被引导。由于该状态存在能隙,电流可以通过静电栅极进行切换。我们的发现可以通过对 Jackiw - Rebbi 模型的推广来解释,其中电子在系统的一个区域中表现为具有有效复质量的费米子,这使得该器件不仅在技术应用方面具有潜力,而且还是高能物理概念的试验场。由密度泛函理论(DFT)计算支持的原子模型表明,该系统可以通过用钛原子修饰石墨烯来实现。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c4/10885192/3b45925e105c/nl3c04703_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c4/10885192/09aafd2bc8c8/nl3c04703_0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c4/10885192/bf65b7b4fa33/nl3c04703_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c4/10885192/5138fb4805eb/nl3c04703_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c4/10885192/aa0e8f47d68d/nl3c04703_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c4/10885192/3b45925e105c/nl3c04703_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c4/10885192/09aafd2bc8c8/nl3c04703_0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c4/10885192/bf65b7b4fa33/nl3c04703_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c4/10885192/5138fb4805eb/nl3c04703_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c4/10885192/aa0e8f47d68d/nl3c04703_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c4/10885192/3b45925e105c/nl3c04703_0005.jpg

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