2016
DOI: 10.1007/s00340-016-6533-6
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A high-efficiency and broadband reflective 90° linear polarization rotator based on anisotropic metamaterial

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Cited by 75 publications
(36 citation statements)
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“…Additionally, most of them have been performed only for monostatic RCSR at normal incident angle ignoring the wave polarization. Hence, nowadays, the modern passive techniques and structures based on phase cancelation or destructive interference using surfaces including frequency selective surface (FSS), 52‐55 EM band gap (EBG), 56‐59 artificial magnetic conductor (AMC), 47,48,60‐77 polarization rotation reflective surface (PRRS), 78‐95 metasurfaces, 96‐145 and hybrid methods, 146‐149 receive a lot of attention to improve the mentioned conventional techniques and overcome their limitations. In the recent decades, researchers have made a lot of efforts on these modern passive RCSR techniques and numerous works have been proposed and completed in order to achieve a system similar to the ideal RCSR system.…”
Section: Introductionmentioning
confidence: 99%
“…Additionally, most of them have been performed only for monostatic RCSR at normal incident angle ignoring the wave polarization. Hence, nowadays, the modern passive techniques and structures based on phase cancelation or destructive interference using surfaces including frequency selective surface (FSS), 52‐55 EM band gap (EBG), 56‐59 artificial magnetic conductor (AMC), 47,48,60‐77 polarization rotation reflective surface (PRRS), 78‐95 metasurfaces, 96‐145 and hybrid methods, 146‐149 receive a lot of attention to improve the mentioned conventional techniques and overcome their limitations. In the recent decades, researchers have made a lot of efforts on these modern passive RCSR techniques and numerous works have been proposed and completed in order to achieve a system similar to the ideal RCSR system.…”
Section: Introductionmentioning
confidence: 99%
“…In addition to the AMC characteristics, the AR bandwidth can be extended with a MS that converts linear polarization (LP) to CP [5][6][7] in the off-band for 3-dB AR. Conversion techniques of polarization to cross polarization [8][9][10][11][12][13][14][15] and from LP to CP [16][17][18][19][20][21][22] have been extensively studied. For example, the principle of the structure in [9] to convert LP to the cross-polarization was explained based on a cut-wire resonator.…”
Section: Introductionmentioning
confidence: 99%
“…Based on various MMs, many different polarization converters have been proposed , and they were usually realized in one of the following two methods: one is to divide a LP wave into two orthogonal components and generate a different phase between them (the fundamental of birefringence effect) by using anisotropic MMs, and the other is to mimic molecule chirality (the fundamental of optical activity) by using chiral MMs. The existing literature indicates that anisotropic two-dimensional MMs (also called metasurfaces) are more suitable for the design of reflective polarizers, and now a number of high-efficiency and ultra-wideband reflective linear polarizers were achieved by using multiple plasmon resonances of different anisotropic metasurfaces [4][5][6][7][8][9][10][11][12][13][14]. However, chiral MMs are convenient for designing transmissive polarizers.…”
Section: Introductionmentioning
confidence: 99%