planar structure
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2022 ◽  
Vol 174 ◽  
pp. 107438
Author(s):  
Linfeng Yu ◽  
Yu Tian ◽  
Xiong Zheng ◽  
Huimin Wang ◽  
Chen Shen ◽  
...  

2021 ◽  
Vol 513 ◽  
pp. 230549
Author(s):  
Xiaofei Hu ◽  
Haichao Yang ◽  
Cong Zhang ◽  
Yanqiao Ding ◽  
Wei Li ◽  
...  

2021 ◽  
Author(s):  
Emiko Horikawa ◽  
Irawati Nurmala Sari ◽  
Weiwei Du

2021 ◽  
pp. 2101219
Author(s):  
Fu Yang ◽  
Lirong Dong ◽  
Dongju Jang ◽  
Begench Saparov ◽  
Kai Cheong Tam ◽  
...  

2021 ◽  
Vol 7 (25) ◽  
pp. eabh0365
Author(s):  
Yanjun Bao ◽  
Long Wen ◽  
Qin Chen ◽  
Cheng-Wei Qiu ◽  
Baojun Li

The Jones matrix is a useful tool to deal with polarization problems, and its number of degrees of freedom (DOFs) that can be manipulated represents its polarization-controlled capabilities. A metasurface is a planar structure that can control light in a desired manner, which, however, has a limited number of controlled DOFs (≤4) in the Jones matrix. Here, we propose a metasurface design strategy to construct a Jones matrix with six DOFs, approaching the upper-limit number of a 2D planar structure. We experimentally demonstrate several polarization functionalities that can only be achieved with high (five or six) DOFs of the Jones matrix, such as polarization elements with independent amplitude and phase tuning along its fast and slow axes, triple-channel complex-amplitude holography, and triple sets of printing-hologram integrations. Our work provides a platform to design arbitrary complex polarization elements, which paves the way to a broader exploitation of polarization optics.


2021 ◽  
Vol 68 (3) ◽  
pp. 1176-1180
Author(s):  
Juan Wang ◽  
Dan Zhao ◽  
Guoqing Shao ◽  
Zhangcheng Liu ◽  
Xiaohui Chang ◽  
...  

Circuit World ◽  
2021 ◽  
Vol ahead-of-print (ahead-of-print) ◽  
Author(s):  
Elakkiya A. ◽  
Radha Sankararajan ◽  
Sreeja B.S.

Purpose The proposed metamaterial absorber (MMA) has the following advantages: first, the structure of the MMA consists of one planar metallic resonator, which presents a new design approach to obtain a multiband absorption response, rather than using multiple unit-cells in the one large unit cell or stacking different layers. Second, the simultaneous realization of triple-band and dual-band absorption (or bi-functional absorption) at five different frequencies can integrate the respective advantages of the triple functions of the triple-band MMA and double-band MMA, and therefore, the bi-functional MMA will find more application prospects than multiple-functional devices of triple-band and dual-band. Third, the authors simulated the three combinations of MMA here, which is indium tin oxide (ITO)-Polyimide-ITO, ITO-Teflon-ITO and ITO-polyethylene terephthalate (PET)-ITO for the same planar structure and achieve a high absorption rate. Finally, the proposed structure is polarization and angle independent in nature. Design/methodology/approach This absorption device consists of the top circular resonator, the middle insulating SiO2 medium layer and the bottom metallic copper ground plane placed on a substrate. The conductivity of the copper metal is s = 5.8 × 107 s/m. As the transmission of the MMA structure is zero, the substrate materials can be selected randomly. Totally four combinations of terahertz MMA are designed and simulated here which are ITO- SiO2 –ITO, ITO-Polyimide-ITO, ITO-Teflon-ITO and ITO- PET-ITO for the same planar structure. Findings Compared with previous MMAs, the proposed MMA has the following advantages: First, the structure of the MMA consists of one planar metallic resonator, which presents a new design approach to obtain a multiband absorption response, rather than using multiple unit-cells in the one large unit cell or stacking different layers. Second, the simultaneous realization of triple-band and dual-band absorption (or bi-functional absorption) at five different frequencies can integrate the respective advantages of the triple functions of the triple-band MMA and double-band MMA, and therefore, the bi-functional MMA will find more application prospects than multiple-functional devices of triple-band and dual-band. Third, the authors simulated the three combinations of MMA here, which is ITO-polyimide-ITO, ITO-Teflon-ITO and ITO- PET-ITO for the same planar structure and achieve a high absorption rate. Finally, the proposed structure is polarization and angle independent in nature. Originality/value First, the structure of the MMA consists of one planar metallic resonator, which presents a new design approach to obtain a multiband absorption response, rather than using multiple unit-cells in the one large unit cell or stacking different layers. Second, the simultaneous realization of triple-band and dual-band absorption (or bi-functional absorption) at five different frequencies can integrate the respective advantages of the triple functions of the triple-band MMA and double-band MMA, and therefore, the bi-functional MMA will find more application prospects than multiple-functional devices of triple-band and dual-band. Third, the authors simulated the three combinations of MMA here, which is ITO-polyimide-ITO, ITO-Teflon-ITO and ITO-PET-ITO for the same planar structure and achieve a high absorption rate. Finally, the proposed structure is polarization and angle independent in nature.


Author(s):  
Zacharias G Fthenakis ◽  
Meghnath Jaishi ◽  
Badri Narayanan ◽  
Antonis N Andriotis ◽  
Madhu Menon

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