1997
DOI: 10.1364/josaa.14.000510
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Resonant excitation of surface modes at a single flat uniaxial–metal interface

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Cited by 25 publications
(17 citation statements)
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“…Tuning the orientation of the dielectric tensor ellipsoid or its principal values was shown to allow tuning of the resonance location. It was shown recently [193,194] that it is possible to excite SP waves directly on the interface of a uniaxial medium and metal. Both TE and TM SP waves were shown to be possible with large sensitivity to the orientation of the optic axis.…”
Section: Laser and Photonics Reviewsmentioning
confidence: 99%
“…Tuning the orientation of the dielectric tensor ellipsoid or its principal values was shown to allow tuning of the resonance location. It was shown recently [193,194] that it is possible to excite SP waves directly on the interface of a uniaxial medium and metal. Both TE and TM SP waves were shown to be possible with large sensitivity to the orientation of the optic axis.…”
Section: Laser and Photonics Reviewsmentioning
confidence: 99%
“…Although the replacement of the isotropic dielectric material by an anisotropic dielectric material has been considered for over three decades [66,67], new understanding continues to emerge [68][69][70][71][72][73]. Equations (2) for the dielectric partnering material then have to be modified to…”
Section: Anisotropic Materialsmentioning
confidence: 99%
“…>°k as for quartz or rutile). Therefore, ¬ 0 may belong to one of three`regions' [24]: Region I, with j¬ 0 =k 0 j > max f…· a°? † 1=2 ; » 1=2 g is the non-radiative region.…”
Section: Regions For the Propagation Constant ¬mentioning
confidence: 99%
“…Previous studies on the modes of structures involving anisotropic media include [11±13] (at a single interface), [14] (the same con®guration as studied here, except that the optic axis of the crystal belongs to the interface, thus excluding double resonances), [15,16] (guided waves in anisotropic media), [17] (two ®lms), [18] (the same structure as considered here, but the study therein does not include double excitations), [19] (®rst observation of enhanced optical secondharmonic generation due to excitation of long-range surface plasmons at a multilayer structure), [20] (multilayered structure, but for a particular orientation of the principal dielectric tensor axes of the anisotropic layer), [21,22] (guided modes in a liquid-crystal layer and surface plasmon resonance in a metal-clad liquid-crystal waveguide respectively), [23,24] (excitation of surface modes at a single uniaxial crystal±metal interface) and [25±28] (examples of excitation at anisotropic gratings). Here we obtain the complex propagation constants of the eigenmodes supported by the uniaxial crystal±metal±isotropic medium ®lm and show the existence of a set of critical ®lm parameters for which the excitation is linked to zeros of the re¯ected power.…”
Section: Introductionmentioning
confidence: 99%