Multi-band, tunable, high figure of merit, high sensitivity single-layer patterned graphene-Perfect absorber based on surface plasmon resonance

被引:71
作者
Chen, Zihao [1 ]
Chen, Hao [1 ]
Yin, Jiankang [2 ]
Zhang, Renyin [1 ]
Jile, Huge [3 ]
Xu, Danyang [4 ]
Yi, Zao [1 ]
Zhou, Zigang [1 ]
Cai, Shuangshuang [5 ]
Yan, Peiguang [6 ]
机构
[1] Southwest Univ Sci & Technol, Sch Natl Def Sci & Technol, Sch Mat Sci & Engn, Sch Sci, Mianyang 621010, Sichuan, Peoples R China
[2] Sichuan Prov Tobacco Co Chengdu Co, Chengdu 610014, Peoples R China
[3] Huzhou Univ, Sch Sci, Huzhou 313000, Peoples R China
[4] Zhejiang Univ Technol, Coll Sci, Hangzhou 310023, Peoples R China
[5] Wenzhou Med Univ, Sch Biomed Engn, Wenzhou 325035, Peoples R China
[6] Shenzhen Univ, Coll Phys & Optoelect Engn, Shenzhen 518060, Peoples R China
基金
中国国家自然科学基金;
关键词
Graphene; Multi-band perfect absorption; High sensitivity; High figure of merit; Tunable; POLARIZATION CONVERTER; METAMATERIAL ABSORBER; INDUCED TRANSPARENCY; MONOLAYER GRAPHENE; TUNGSTEN DISULFIDE; PULSE GENERATION; ABSORPTION; HETEROJUNCTION;
D O I
10.1016/j.diamond.2021.108393
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
This paper propose a perfect absorber with multi-band, adjustable, high figure of merit (FOM) and high sensitivity is based on single-layer patterned graphene surface plasmon resonance (SPR). The wave absorber is composed of a patterned graphene structure etched in a circular shape in the middle and a bottom metal film separated by a SiO2 dielectric layer. It has simple structural features and can greatly simplify the manufacturing process. In the mid-infrared band of 3 mu m similar to 5 mu m, the numerical results of FDTD method show that the absorbers have three perfect absorption peaks, which are lambda(1) = 3275.31 nm, lambda(2) = 3706.12 nm and lambda(3) = 4481.76 nm, respectively. The absorption rates are 99.44%, 98.22% and 99.10%, respectively. The resonant wavelength of the absorber can be tuned by controlling the Fermi energy level and relaxation time of the graphene layer. In addition, the wave absorber is insensitive to polarization and can keep high absorption in a wide range of incident angles from 0 degrees to 50 degrees. At last, we explore the sensitivity and FOM of the absorber by changing the environmental refractive index. The results show that the sensitivity of its three resonance absorption peaks is 666.75 nm/RIU, 760.50 nm/RIU and 907.88 nm/RIU (RIU is the per refractive index unit), and the FOM is 86.82, 53.03 and 56.14, respectively. Therefore, we believe that the absorber can be used in the fields of narrowband thermal radiation, narrow-band light detection and narrow-band sensor.
引用
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页数:8
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