4.6 Article

A perfect absorber of multi-band, tunable monolayer patterned graphene based on surface plasmon resonance

Journal

DIAMOND AND RELATED MATERIALS
Volume 130, Issue -, Pages -

Publisher

ELSEVIER SCIENCE SA
DOI: 10.1016/j.diamond.2022.109498

Keywords

Graphene; Tunable; Multi-band perfect absorption; FDTD solution

Funding

  1. National Natural Science Foundation of China [51606158, 11604311, 61705204, 21506257]
  2. Scientific Research Fund of Si Chuan Provincial Science and Technology Department [2020YJ0137, 2020YFG0467]
  3. Opening Project of Key Laboratory of Microelectronic Devices & Integrated Technology, Institute of Micro-electronics, Chinese Academy of Sciences
  4. College Students' Innovation and Entrepreneurship Training program [S202110619100]
  5. Undergraduate Innovation Fund Project Precision Funding by Southwest University of Science and Technology [JZ22-080]

Ask authors/readers for more resources

This article investigates and proposes a triple-band ultra-perfect absorber based on graphene surface plasmon resonance. By using the finite difference time domain (FDTD) method, three perfect absorption peaks in the mid-infrared wavelength range are identified. The paper shows that the absorption peak can be controlled by changing the Fermi energy level and relaxation time of graphene, and the absorbed resonant waves can also be controlled by adjusting the refractive index of the environment and SiO2. The absorber exhibits polarisation and angle insensitivity, maintaining high absorption for different incident angles. The simulations reveal three resonance absorption peaks with sensitivities, indicating the potential value of the absorber in various applications.
A triple-band ultra-perfect absorber with tunability based on graphene surface plasmon resonance is investigated and proposed in this article. According to the finite difference time domain (FDTD) method, in the mid-infrared wavelength range of 3400 nm -4000 nm, we have identified three perfect absorption peaks, namely at lambda 1 = 3548.54 nm, lambda 2 = 3660.25 nm and lambda 3 = 3912.99 nm, in which the absorption rate 99.90 %, 99.05 %, 99.13 % respectively. By discussing different graphene geometries, this paper shows the best results of this experiment. If we want to control the amplitude of the absorption peak and the wavelength of the resonance, we can do so in two ways: first, by changing the Fermi energy level of the graphene, and second, by changing the relaxation time of the graphene. Besides, the absorbed resonant waves can slao be controlled by adjusting the refractive index of the environment in which they are located and the refractive index of SiO2. The absorber exhibits polarisation and angle insensitivity, so when the angle of incidence varies in the (0 degrees -50 degrees) range, the absorber we have designed also maintains high absorption. Three resonance absorption peaks with sensitivities of 845.7 nm/RIU, 880.3 nm/RIU and 942.6 nm/RIU can be obtained from the results of the simulations. In summary, we believe that the absorber with its various characteristics could be of great value in a number of applications.

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