Dual‐band Absorption Effect in a Topological Insulator Based Tamm Plasmon Multilayer System

Author(s):  
Meghna C H ◽  
Vincent Mathew
2021 ◽  
pp. 104747
Author(s):  
Haixia Liu ◽  
Shashi Zhang ◽  
Hao Ding ◽  
Wei Sun ◽  
Lichen Sun

Author(s):  
A. G. Mignani ◽  
L. Ciaccheri ◽  
A. A. Mencaglia ◽  
J. Xing ◽  
X. Yang ◽  
...  

2018 ◽  
Vol 34 (5) ◽  
pp. 772-780 ◽  
Author(s):  
Yuping Che ◽  
Yang Wang ◽  
Tingting You ◽  
Huaiqiu Chang ◽  
Penggang Yin ◽  
...  

2016 ◽  
Vol 120 (20) ◽  
pp. 205103 ◽  
Author(s):  
Debidas Kundu ◽  
Akhilesh Mohan ◽  
Ajay Chakrabarty
Keyword(s):  

2019 ◽  
Vol 68 (22) ◽  
pp. 224301
Author(s):  
Ding Jia ◽  
Yong Ge ◽  
Shou-Qi Yuan ◽  
Hong-Xiang Sun

Materials ◽  
2018 ◽  
Vol 11 (11) ◽  
pp. 2193 ◽  
Author(s):  
Taiguo Lu ◽  
Dawei Zhang ◽  
Peizhen Qiu ◽  
Jiqing Lian ◽  
Ming Jing ◽  
...  

We designed an ultra-thin dual-band metamaterial absorber by adjusting the side strips’ length of an H-shaped unit cell in the opposite direction to break the structural symmetry. The dual absorption peaks approximately 99.95% and 99.91% near the central resonance frequency of 4.72 THz and 5.0 THz were obtained, respectively. Meanwhile, a plasmon-induced transmission (PIT) like reflection window appears between the two absorption frequencies. In addition to theoretical explanations qualitatively, a multi-reflection interference theory is also investigated to prove the simulation results quantitatively. This work provides a way to obtain perfect dual-band absorption through an asymmetric metamaterial structure, and it may achieve potential applications in a variety of fields including filters, sensors, and some other functional metamaterial devices.


2013 ◽  
Vol 102 (8) ◽  
pp. 081122 ◽  
Author(s):  
P. V. Tuong ◽  
J. W. Park ◽  
J. Y. Rhee ◽  
K. W. Kim ◽  
W. H. Jang ◽  
...  

2014 ◽  
Vol 28 (14) ◽  
pp. 1450109 ◽  
Author(s):  
Yan-Lin Liao ◽  
Yan Zhao

In this paper, a wide-angle polarization-sensitive dual-band absorber at infrared wavelengths with a multilayer grating is reported. The simulation results show that the absorber has two absorption peaks at wavelengths λ = 1.365 μ m and λ = 3.035 μ m with the absorption magnitudes more than 0.97 and 0.99 for TM polarization (electric field perpendicular to the strips), respectively. And this absorber reflects almost all TE polarization (electric field parallel to the strips) light. The dual-band absorption peaks can be tuned by varying the width of the strips, and the absorption magnitudes are more than 0.9 for the dual-band absorption peaks for angles up to 70°.


2013 ◽  
Vol 38 (7) ◽  
pp. 1125 ◽  
Author(s):  
Nan Zhang ◽  
Peiheng Zhou ◽  
Dengmu Cheng ◽  
Xiaolong Weng ◽  
Jianliang Xie ◽  
...  

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