Polarization- and angle-insensitive ultrabroadband perfect metamaterial absorber for thermophotovoltaics

2021 ◽  
Vol 38 (2) ◽  
pp. 327
Author(s):  
Ashish Kumar Chowdhary ◽  
Tanmay Bhowmik ◽  
Debabrata Sikdar
2021 ◽  
Vol 23 ◽  
pp. 104037
Author(s):  
Miao Pan ◽  
Huazhu Huang ◽  
Baodian Fan ◽  
Wenzhi Chen ◽  
Shuai Li ◽  
...  

Nanophotonics ◽  
2021 ◽  
Vol 10 (4) ◽  
pp. 1337-1346
Author(s):  
Jin Tao ◽  
Zhongzhu Liang ◽  
Guang Zeng ◽  
Dejia Meng ◽  
David R. Smith ◽  
...  

Abstract Cointegration and coupling a perfect metamaterial absorber (PMA) together with a film bulk acoustic wave resonator (FBAR) in a monolithic fashion is introduced for the purpose of producing ultracompact uncooled infrared sensors of high sensitivity. An optimized ultrathin multilayer stack was implemented to realize the proposed device. It is experimentally demonstrated that the resonance frequency of the FBAR can be used efficiently as a sensor output as it downshifts linearly with the intensity of the incident infrared irradiation. The resulting sensor also achieves a high absorption of 88% for an infrared spectrum centered at a wavelength of 8.2 μm. The structure is compact and can be easily integrated on a CMOS-compatible chip since both the FBAR and PMA utilize and share the same stack of metal and dielectric layers.


2016 ◽  
Vol 24 (2) ◽  
pp. 1518 ◽  
Author(s):  
Gang Yao ◽  
Furi Ling ◽  
Jin Yue ◽  
Chunya Luo ◽  
Jie Ji ◽  
...  

2019 ◽  
Vol 15 ◽  
pp. 102760 ◽  
Author(s):  
Yuyin Li ◽  
Qiqi Chen ◽  
Biao Wu ◽  
Leilei Shi ◽  
Peng Tang ◽  
...  

2019 ◽  
Vol 33 (36) ◽  
pp. 1950460 ◽  
Author(s):  
Xiaojie Lu ◽  
Zhongyin Xiao ◽  
Mingming Chen

In this work, we present the analysis and design of a perfect metamaterial absorber (MA) based on quarter mode rectangular cavity in the terahertz region. This structure is consisted of a metal plate where three different size quarter mode rectangular cavities are vertically placed on. Based on rectangular-cavity-theory, a formula is proposed to calculate the resonant frequency, which provides a guidance for designing MAs of such type. In terms of normal incidence, the simulated results show that the MA has three resonance points on 4.1301 THz, 4.6051 THz and 5.1088 THz, respectively, which is in good agreement with the calculated results. Furthermore, we present the distribution of E-field in the cavity and use the standing wave theory to explain the physical mechanism of the perfect absorption. These results verify the application of resonant cavities in the field of MA.


2019 ◽  
Vol 14 ◽  
pp. 102463 ◽  
Author(s):  
Chunlian Cen ◽  
Zao Yi ◽  
Guangfu Zhang ◽  
Yubin Zhang ◽  
Cuiping Liang ◽  
...  

2017 ◽  
Vol 49 (1) ◽  
Author(s):  
B. Ni ◽  
Z. Y. Wang ◽  
R. S. Zhao ◽  
X. Y. Ma ◽  
Z. Q. Xing ◽  
...  

2016 ◽  
Vol 46 (1) ◽  
pp. 413-417 ◽  
Author(s):  
Manh Cuong Tran ◽  
Thi Thuy Nguyen ◽  
Tuan Hung Ho ◽  
Hoang Tung Do

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