2020
DOI: 10.5802/crmath.59
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Electromagnetic shielding by thin periodic structures and the Faraday cage effect

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Cited by 4 publications
(4 citation statements)
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“…Remark A.1.For the sake of conciseness, the proof of the existence and uniqueness of Q − and Q + is not written here (e.g. [8]). It is based on the application of the Lax–Milgram lemma together with a Hardy equality [19, lemma 2.5.7].…”
Section: Figure 16mentioning
confidence: 99%
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“…Remark A.1.For the sake of conciseness, the proof of the existence and uniqueness of Q − and Q + is not written here (e.g. [8]). It is based on the application of the Lax–Milgram lemma together with a Hardy equality [19, lemma 2.5.7].…”
Section: Figure 16mentioning
confidence: 99%
“…Indeed, for thick wires with ( e / h ) = O (1), the coupling cannot be captured by the limit problem; at zero order, the array is crudely replaced by a Dirichlet wall. (In [8], this is used to discriminate between different geometries of arrays producing an efficient shielding.) The coupling is captured at the first order.…”
Section: Introductionmentioning
confidence: 99%
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“…If the whole machine debugging and performance appraisal of the radar adopts field test, real targets (such as rockets and satellites) are used to provide test signals to the radar, financial, and material resources and increase the development cost. When the energy of the incident ray photon exceeds 1.02 MeV (equivalent to 2 times the rest mass of the electron), there will be a positive-negative electron pair effect, that is, the incident high-energy photon forms a positive-negative electron pair in the Coulomb field of the material nucleus with the energy equal to the incident photon energy [15,16].…”
Section: Electromagnetic Occlusion Algorithmmentioning
confidence: 99%