2018
DOI: 10.1088/1361-6463/aab0c2
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Extremely high contrast asymmetric transmission with linear tunability in chiral metamaterials

Abstract: In this paper, asymmetric transmission with extremely high contrast for linear polarization is proposed in chiral split ring resonators. Results show that only specific cross-polarization can pass through the structure with a high power transmission efficiency of 0.9 (amplitude transmission 0.95), which is much higher than those reported before in infrared region. The contrast between the two cross-polarizations is also very large (larger than 24.5 dB). Another merit of our scheme is that the operation wavelen… Show more

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Cited by 15 publications
(6 citation statements)
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“…Fortunately, the emergence of metamaterial provides an appealing alternative to control electromagnetic wave manipulations properties [12][13][14][15][16][17], and the discovery of the AT phenomenon based on metamaterial was first experimentally demonstrated in the microwave region by Fedotov et al in 2006 [18]. Since then, various AT devices based on artificial structures have been proposed which use photonic crystals [19,20], subwavelength asymmetric gratings [21][22][23][24], chiral metamaterials [25][26][27] and metasurfaces [28][29][30], and the operation wavelengths have been covered from microwave to visible light [31][32][33]. These devices show promise to some degree; however, those using chiral metamaterials are usually complex and incorporate multilayer structures, whereas those using subwavelength asymmetric gratings are polarization sensitive.…”
Section: Introductionmentioning
confidence: 99%
“…Fortunately, the emergence of metamaterial provides an appealing alternative to control electromagnetic wave manipulations properties [12][13][14][15][16][17], and the discovery of the AT phenomenon based on metamaterial was first experimentally demonstrated in the microwave region by Fedotov et al in 2006 [18]. Since then, various AT devices based on artificial structures have been proposed which use photonic crystals [19,20], subwavelength asymmetric gratings [21][22][23][24], chiral metamaterials [25][26][27] and metasurfaces [28][29][30], and the operation wavelengths have been covered from microwave to visible light [31][32][33]. These devices show promise to some degree; however, those using chiral metamaterials are usually complex and incorporate multilayer structures, whereas those using subwavelength asymmetric gratings are polarization sensitive.…”
Section: Introductionmentioning
confidence: 99%
“…It requires the symmetry in the z direction to be broken, and chiral structures are commonly utilized to achieve this goal [26,28,36], which is the basis of our design. It should be stressed that the AT phenomenon here are reciprocal in physics.…”
Section: Methodsmentioning
confidence: 99%
“…In addition, the use of multilayer metallic configurations prevents obtaining a highcontrast AT ratio. Although optical devices with an AT characteristic can be realized using plasmonic metamaterials as another approach [5][6][7], they usually exhibit low transmission amplitudes due to optical losses in the multilayer designs [14][15][16][17][18][19][20]. Moreover, the realization of a double grating design separated by a thin dielectric is a challenging task from the fabrication perspective [21][22][23].…”
Section: Introductionmentioning
confidence: 99%