2018
DOI: 10.1103/physrevx.8.031077
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Huygens’ Metadevices for Parametric Waves

Abstract: Huygens' metasurfaces have demonstrated almost arbitrary control over the shape of a scattered beam, however its spatial profile is typically fixed at fabrication time. Dynamic reconfiguration of this beam profile with tunable elements remains challenging, due to the need to maintain the Huygens' condition across the tuning range. In this work, we experimentally demonstrate that a time-varying meta-device which performs frequency conversion, can steer transmitted or reflected beams in an almost arbitrary manne… Show more

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Cited by 143 publications
(183 citation statements)
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References 70 publications
(71 reference statements)
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“…Note that, in the raised relaxation oscillation, the second laser spike is stronger than the first one, contrary to the damped relaxation oscillation where the second one is weaker than the first one. [15,57] Each laser spike contains a large number of sub-nanosecond pulses, as shown in Figure 3a. The obvious beating behavior is observed from 1.9 × 10 4 to 2.08 × 10 4 RTs.…”
Section: Resultsmentioning
confidence: 99%
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“…Note that, in the raised relaxation oscillation, the second laser spike is stronger than the first one, contrary to the damped relaxation oscillation where the second one is weaker than the first one. [15,57] Each laser spike contains a large number of sub-nanosecond pulses, as shown in Figure 3a. The obvious beating behavior is observed from 1.9 × 10 4 to 2.08 × 10 4 RTs.…”
Section: Resultsmentioning
confidence: 99%
“…Figure 5a illustrates the Fourier transform of each single-shot spectrum in Figure 2b, corresponding to a field autocorrelation of the momentary pulses, which traces the evolution of temporal separation between pulses. [15,51] Figures 5b and 5c are enlarge-ments of the A and B regions in Figure 5a Figure 4b,c), and in succession, weaker modulation instability is induced by SPM. [58] The SPM-induced instability gradually increases until 1.06 × 10 5 RTs (an example is shown as black curves in Figure 4b,c), finally leading to the pulse splitting which gives birth to five pulses, as shown in Figure 5c.…”
Section: Resultsmentioning
confidence: 99%
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“…To solve the problem of fixed wave-manipulations by passive metasurfaces, more efforts have been devoted to realize active control of EM behaviors of metasurfaces upon the external stimulations by incorporating with tunable materials or components, [30,31] such as diodes, [32][33][34][35] graphene, [36,37] phase-change materials, [38,39] etc. Recently, coding metasurfaces have been proposed to control the wave functionalities using unique particles with, for example, either the "0" or "1" state in 1-bit coding case.…”
mentioning
confidence: 99%
“…linearly polarized excitation, [32][33][34][35][36][37][38] leaving much potentials unexploited. Undoubtedly, the active anisotropic metasurfaces for independent dual-polarized manipulations of EM waves will further increase their information capabilities, bringing new degrees of freedom in achieving versatile tunable functionalities that are highly desirable from application aspects.…”
mentioning
confidence: 99%