4.5 Article

Dynamically tunable multiband plasmon-induced transparency effect based on graphene nanoribbon waveguide coupled with rectangle cavities system

Journal

CHINESE PHYSICS B
Volume 31, Issue 8, Pages -

Publisher

IOP Publishing Ltd
DOI: 10.1088/1674-1056/ac7e39

Keywords

plasmon-induced transparency (PIT); graphene; group index; rectangle cavities

Funding

  1. National Natural Science Foundation of China [11647122, 61705064]
  2. Natural Science Foundation of Hubei Province, China [2018CFB672, 2021CFB607]
  3. Project of the Hubei Provincial Department of Education, China [B2021215, T201617]
  4. Natural Science Foundation of Xiaogan City, China [XGKJ2021010002, XGKJ2021010003]

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In this study, a dynamically tunable multiband plasmon-induced transparency (PIT) effect is investigated using a graphene nanoribbon waveguide system coupled with rectangle cavities. Single-PIT effect is achieved through destructive interference and indirect coupling, while dual-PIT effect is obtained by side-coupling three rectangle cavities with a graphene nanoribbon waveguide. The combination of bright-dark mode coupling and cavities side-coupled with waveguide mechanism leads to triple-PIT effect. This research introduces a novel approach for the realization of optical sensors, filters, and slow light devices with ultra-compact and dynamic tunable characteristics.
A dynamically tunable multiband plasmon-induced transparency (PIT) effect in a series of rectangle cavities coupled with a graphene nanoribbon waveguide system is investigated theoretically and numerically by tuning the Fermi level of the graphene rectangle cavity. A single-PIT effect is realized using two different methods: one is the direct destructive interference between bright and dark modes, and the other is the indirect coupling through a graphene nanoribbon waveguide. Moreover, dual-PIT effect is obtained by three rectangle cavities side-coupled with a graphene nanoribbon waveguide. Results show that the magnitude of the dual-PIT window can be controlled between 0.21 and 0.74, and the corresponding group index is controlled between 143.2 and 108.6. Furthermore, the triple-PIT effect is achieved by the combination of bright-dark mode coupling and the cavities side-coupled with waveguide mechanism. Thus, sharp PIT windows can be formed, a high transmission is maintained between 0.51 and 0.74, and the corresponding group index is controlled between 161.4 and 115.8. Compared with previously proposed graphene-based PIT effects, the size of the introduced structure is less than 0.5 mu m(2). Particularly, the slow light effect is crucial in the current research. Therefore, a novel approach is introduced toward the realization of optical sensors, optical filters, and slow light and light storage devices with ultra-compact, multiband, and dynamic tunable.

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