Six-band terahertz metamaterial absorber based on the combination of multiple-order responses of metallic patches in a dual-layer stacked resonance structure
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作者:
Wang, Ben-Xin
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Jiangnan Univ, Sch Sci, Jiangsu Prov Res Ctr Light Ind Optoelect Engn & T, Wuxi 214122, Peoples R ChinaJiangnan Univ, Sch Sci, Jiangsu Prov Res Ctr Light Ind Optoelect Engn & T, Wuxi 214122, Peoples R China
Wang, Ben-Xin
[1
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Wang, Gui-Zhen
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Hunan Tradit Chinese Med Coll, Lib & Informat Ctr, Zhuzhou 412012, Peoples R ChinaJiangnan Univ, Sch Sci, Jiangsu Prov Res Ctr Light Ind Optoelect Engn & T, Wuxi 214122, Peoples R China
Wang, Gui-Zhen
[2
]
Sang, Tian
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Jiangnan Univ, Sch Sci, Jiangsu Prov Res Ctr Light Ind Optoelect Engn & T, Wuxi 214122, Peoples R ChinaJiangnan Univ, Sch Sci, Jiangsu Prov Res Ctr Light Ind Optoelect Engn & T, Wuxi 214122, Peoples R China
Sang, Tian
[1
]
Wang, Ling-Ling
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Hunan Univ, Sch Phys & Electron, Changsha 410082, Hunan, Peoples R ChinaJiangnan Univ, Sch Sci, Jiangsu Prov Res Ctr Light Ind Optoelect Engn & T, Wuxi 214122, Peoples R China
Wang, Ling-Ling
[3
]
机构:
[1] Jiangnan Univ, Sch Sci, Jiangsu Prov Res Ctr Light Ind Optoelect Engn & T, Wuxi 214122, Peoples R China
[2] Hunan Tradit Chinese Med Coll, Lib & Informat Ctr, Zhuzhou 412012, Peoples R China
[3] Hunan Univ, Sch Phys & Electron, Changsha 410082, Hunan, Peoples R China
This paper reports on a numerical study of the six-band metamaterial absorber composed of two alternating stack of metallic-dielectric layers on top of a continuous metallic plane. Six obvious resonance peaks with high absorption performance (average larger than 99.37%) are realized. The first, third, fifth, and the second, fourth, sixth resonance absorption bands are attributed to the multiple-order responses (i.e., the 1-, 3-and 5-order responses) of the bottom-and top-layer of the structure, respectively, and thus the absorption mechanism of six-band absorber is due to the combination of two sets of the multiple-order resonances of these two layers. Besides, the size changes of the metallic layers have the ability to tune the frequencies of the six-band absorber. Employing the results, we also present a six-band polarization tunable absorber through varying the sizes of the structure in two orthogonal polarization directions. Moreover, nine-band terahertz absorber can be achieved by using a three-layer stacked structure. Simulation results indicate that the absorber possesses nine distinct resonance bands, and average absorptivities of them are larger than 94.03%. The six-band or nine-band absorbers obtained here have potential applications in many optoelectronic and engineering technology areas.