2018
DOI: 10.1016/j.optcom.2017.12.036
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Broadband tunable terahertz polarization converter based on graphene metamaterial

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Cited by 49 publications
(21 citation statements)
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“…Due to its unique electrical and optical properties in the terahertz and mid-infrared regimes, many intriguing applications have been proposed, such as the optical devices, plasmon waveguiding, clocking devices and many other optoelectronic applications. Compared with metal plasmonics with restricted flexible permittivity, the most remarkable advantage of the graphene is its capability of dynamically tuning the conductivity through straightforward chemical or electrostatic gatings, which opens the door to many exciting tunable devices, such as tunable absorbers [24][25][26][27][28][29][30], and tunable polarization converters [31][32][33][34][35][36][37][38][39][40]. For example, Cheng et al proposed a dynamically tunable broadband cross polarization converter (CPC) made of L-shaped graphene sheets, which transformed linear light into cross polarization light for a single band in the midinfrared regions [31].…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…Due to its unique electrical and optical properties in the terahertz and mid-infrared regimes, many intriguing applications have been proposed, such as the optical devices, plasmon waveguiding, clocking devices and many other optoelectronic applications. Compared with metal plasmonics with restricted flexible permittivity, the most remarkable advantage of the graphene is its capability of dynamically tuning the conductivity through straightforward chemical or electrostatic gatings, which opens the door to many exciting tunable devices, such as tunable absorbers [24][25][26][27][28][29][30], and tunable polarization converters [31][32][33][34][35][36][37][38][39][40]. For example, Cheng et al proposed a dynamically tunable broadband cross polarization converter (CPC) made of L-shaped graphene sheets, which transformed linear light into cross polarization light for a single band in the midinfrared regions [31].…”
Section: Introductionmentioning
confidence: 99%
“…For example, Cheng et al proposed a dynamically tunable broadband cross polarization converter (CPC) made of L-shaped graphene sheets, which transformed linear light into cross polarization light for a single band in the midinfrared regions [31]. Nanocross has also been used in to efficiently convert the polarization states [32], [34]. Other structures, such as Hollow-Carved "H" Array [41], butterfly-shaped holes [42], have also been demonstrated to be suitable to achieve high polarization conversion efficiency.…”
Section: Introductionmentioning
confidence: 99%
“…Thanks to the extremely thin thickness of only 0.34 nm, graphene can be regarded as an infinitely thin twodimensional planar material and ignores the edge effect. In the midst of this situation, the surface conductivity δ s (ω, µ c , , T ) based on the Kubo formula [18] are investigated to characterize the peculiar electronic properties of graphene. In general, δ s (ω, µ c , , T ) mainly consists two parts which are intraband contributions δ intra (ω, µ c , , T ) and interband contributions δ inter (ω, µ c , , T ), respectively, as shown in Eqs.…”
Section: Design and Simulationmentioning
confidence: 99%
“…In 2013, Cheng et al [17] proposed an tunable cross polarization converter based on L-shaped graphene nanostructures, which offered a further step in developing for dynamic reconfigurable devices. Similarly, a cross-polarization converter with the bandwidth of 25.8% is designed by Luo et al [18] and such a bandwidth can be regulated by controlling the E f of graphene sheets. With the development of graphene devices, it will have broader potential applications in various fields such as antennas [19], [20], filters [21], [22] and phase shifters [23].…”
Section: Introductionmentioning
confidence: 99%
“…Graphene, a two-dimensional carbon material, has been widely employed to configure polarization conversion metamaterials [23]- [30] due to its excellent ability of dynamically controlling the Fermi energy. Bulk Dirac semimetal (BDS), the material performs like the "three-dimensional (3D) graphene", has been introduced in metamaterial design [31]- [34].…”
Section: Introductionmentioning
confidence: 99%