Non-left-handed transmission and bianisotropic effect in a [pi]-shaped metallic metamaterials

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dc.creatorDong, Z. G.
dc.creatorLei, S. Y.
dc.creatorLi, Q.
dc.creatorXu, M. X.
dc.creatorLiu, H.
dc.creatorLi, T.
dc.creatorWang, F. M.
dc.creatorZhu, S. N.
dc.date2007-02-23
dc.date2007-02-24
dc.date.accessioned2026-07-07T07:48:25Z
dc.date.available2026-07-07T07:48:25Z
dc.descriptionA [pi]-shaped metallic metamaterial (geometrically, a combination medium of C-shaped resonators and continuous wires) is proposed to numerically investigate its transmission band near the resonant frequency, where otherwise it should be a negative-permeability (or negative-permittivity) stop band if either the C-shaped or continuous-wire constituent is separately considered. However, in contrast to the left-handed materials (LHMs)composed of split-ring resonators and wires as well as other metallic LHMs, this resonant transmission is a non-left-handed one as a result of the intrinsic bianisotropic effect attributed to the electrically asymmetric configuration of this [pi]-shaped metamaterial.
dc.description19 pages, 6 figures
dc.identifierhttps://arxiv.org/abs/cond-mat/0702547
dc.identifierhttp://arxiv.org/abs/cond-mat/0702547
dc.identifierPHYSICAL REVIEW B 75, 075117(2007)
dc.identifierdoi:10.1103/PhysRevB.75.075117
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/124492
dc.subjectMesoscale and Nanoscale Physics
dc.subjectOther Condensed Matter
dc.titleNon-left-handed transmission and bianisotropic effect in a [pi]-shaped metallic metamaterials
dc.typetext

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