2020
DOI: 10.1016/j.optcom.2020.125333
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Single- and dual-band convertible terahertz absorber based on bulk Dirac semimetal

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Cited by 21 publications
(12 citation statements)
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“…In addition, the electromagnetic field energy distribution of the terahertz absorber is clearly explained by FEM. Compared with the reported terahertz absorber, [ 27 ] the terahertz metamaterial absorber in our work has the angle‐insensitive and tunable characteristics. In addition, the results show that the absorber designed has good fabrication tolerance.…”
Section: Discussionmentioning
confidence: 86%
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“…In addition, the electromagnetic field energy distribution of the terahertz absorber is clearly explained by FEM. Compared with the reported terahertz absorber, [ 27 ] the terahertz metamaterial absorber in our work has the angle‐insensitive and tunable characteristics. In addition, the results show that the absorber designed has good fabrication tolerance.…”
Section: Discussionmentioning
confidence: 86%
“…Meanwhile, the terahertz absorber achieves a dual-broadband absorption peak of 94.56% and 99.11% at 11.4 and 26.2 THz, respectively. Compared with the reported terahertz absorber, [27] the graphene-based absorber in our work can adjust the Fermi level to achieve the tunable and angle-insensitive absorption peak. In addition, in contrast to other reported graphene-based dual-band absorbers, [28][29][30] our proposed structure is simple and does not require patterning in graphene, which does not cause unnecessary contamination and damage to ultrathin graphene and reduces the fabrication difficulty in the actual production process.…”
Section: Introductionmentioning
confidence: 99%
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“…Topological materials (TMs) ( Cava et al, 2013 ; Kong and Cui, 2011 ; Xu et al, 2015 ; Strambini et al, 2016 ; Wang et al, 2017 ; Banik et al, 2018 ; Kageyama et al, 2018 ; Schoop et al, 2018 ; Culcer et al, 2020 ; Kumar et al, 2020 ; Li and Xia, 2020 ; Xu et al, 2020 ) enjoy nontrivial band-crossings (BCs) in their low-energy region, giving rise to novel fermionic excitations. A series of TMs, including nodal-point ( Alcón et al, 2017 ; Fu et al, 2018a ; Kong et al, 2018 ; Jin et al, 2019a ; Jin et al, 2019b ; Wang et al, 2019 ; Fang et al, 2020 ; Zhang et al, 2020 ), nodal-line ( Chen et al, 2018 ; Zhou et al, 2018 ; Li et al, 2019 ; Liu et al, 2019 ; Sankar et al, 2019 ; Tang et al, 2019 ; Xu et al, 2019 ; Yi et al, 2019 ; Wang et al, 2020a ; Zhao et al, 2020 ), and nodal-surface ( Wu et al, 2018 ; Qie et al, 2019 ; Wang et al, 2020b ) materials, have been predicted via symmetry and first-principle analysis. Some of them have been verified via experiment.…”
Section: Introductionmentioning
confidence: 99%
“…Similarly, the relative permittivity of BDS, a material that can be considered as “3D graphene”, can also be dynamically controlled by an external gate voltage [ 8 , 9 ]. Up to now, some graphene- or Dirac-semimetal-based devices have been reported in the terahertz range [ 10 , 11 , 12 , 13 , 14 , 15 , 16 , 17 , 18 ]. Nevertheless, the bandwidth of these absorbers is not wide enough, and the tuning method is relatively monotonous.…”
Section: Introductionmentioning
confidence: 99%