2010
DOI: 10.1088/1367-2630/12/4/043046
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Sum rules and physical bounds on passive metamaterials

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Cited by 54 publications
(100 citation statements)
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References 28 publications
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“…With a "normal" surrounding medium having a permittivity function with { } > 0, this requires a permittivity function for the interior region with a negative real part { 1 } < 0, a material property that sometimes is associated with a metamaterial and which may have severe limitations on the bandwidth capabilities, cf., [22].…”
Section: Narrowband Realizability Of the Conjugate Match: Tuning Thementioning
confidence: 99%
“…With a "normal" surrounding medium having a permittivity function with { } > 0, this requires a permittivity function for the interior region with a negative real part { 1 } < 0, a material property that sometimes is associated with a metamaterial and which may have severe limitations on the bandwidth capabilities, cf., [22].…”
Section: Narrowband Realizability Of the Conjugate Match: Tuning Thementioning
confidence: 99%
“…Similar physical bounds restricting the performance of passive structures have been presented in several papers treating matching methods [5], nite size scatterers [10,2628], antennas [8,9], absorbers [18], articial magnetic ground planes [4], and metamaterials [7,25,29]. A common factor for all these bounds, is that the integrated electromagnetic interaction of the scatterer, antenna, or material, is bounded by the static properties of the system.…”
Section: Introductionmentioning
confidence: 58%
“…It is also noted that the parameters of a Drude model can always be tuned to the conjugate match at a single frequency, but just like the metamaterials with real valued and negative permittivity [2], the conjugate match (with small imaginary part) is not realizable as a passive material over a finite bandwidth, cf., [4].…”
Section: Optimal Absorption For the Spherementioning
confidence: 99%
“…In Figure 1 is shown the absorption cross section C abs given by (2), plotted as a function of frequency and where the radius of the spherical suspension is r 1 = 1 µm. In Figure 2 is shown the relative heating coefficient F a (ε 1 ) given by (1) representing the mean power dissipation inside a small sphere relative the mean power dissipation in a close vicinity of the sphere.…”
Section: Optimal Absorption For the Spherementioning
confidence: 99%