2020
DOI: 10.1109/tap.2019.2948528
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Active Scattering-Cancellation Cloaking: Broadband Invisibility and Stability Constraints

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Cited by 26 publications
(14 citation statements)
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“…In particular, the resonance frequency ω 0 and the ratio of plasma frequency ω p to ω 0 for this additional resonance should be large with respect to the original two inverted Lorentzian resonances, in order for the refractive index of the cloaking material to remain approximately dispersionless and between zero and unity in the frequency range of interest. This modified, causal, material dispersion, however, typically leads to an unstable scattering response 18 , characterized by the onset of unbounded temporal oscillations (corresponding to unstable scattering poles), as shown in Fig. 2 c, d and the Supplementary video .…”
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confidence: 99%
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“…In particular, the resonance frequency ω 0 and the ratio of plasma frequency ω p to ω 0 for this additional resonance should be large with respect to the original two inverted Lorentzian resonances, in order for the refractive index of the cloaking material to remain approximately dispersionless and between zero and unity in the frequency range of interest. This modified, causal, material dispersion, however, typically leads to an unstable scattering response 18 , characterized by the onset of unbounded temporal oscillations (corresponding to unstable scattering poles), as shown in Fig. 2 c, d and the Supplementary video .…”
mentioning
confidence: 99%
“…In the context of cloaking, gain media, fast-light media, and so-called non-Foster circuits (active circuits implementing negative resistances, capacitances, inductances) have already been proposed, years before ref. 1 , to realize invisibility cloaks that, while not perfect and still constrained by causality, are indeed more broadband and efficient than their passive counterparts 17 , 18 . Yet, there are several limits and design considerations that must be taken into account and deserve further discussion.…”
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confidence: 99%
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