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Mode recombination and alternation of surface plasmons in anisotropic mediums
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View: Figures


Image of FIG. 1.
FIG. 1.

The schematic diagram of the three-layer dielectric-metal-anisotropic plasmon structure with the optical axis of anisotropic medium in the yz or the xz plane.

Image of FIG. 2.
FIG. 2.

Propagation constants as functions of for the gold film thickness d = 50 nm, d = 70 nm, and d = 80 nm, respectively. Inset (a): the amplified figure for d = 70 nm near ; inset (b): the profile of the squared modulus of complex electric field at , where the value is normalized by that at x = −40 nm, the lower interface. Here, for the LC, and .

Image of FIG. 3.
FIG. 3.

The propagation constants as a function of for d = 80 nm, 100 nm, and 130 nm, respectively. The parameters are the same as those in Fig. 2 , except that and the OA of the LC is in the xz plane.

Image of FIG. 4.
FIG. 4.

The profiles of energy flux at the points and (i = 1, 2, 3), which are denoted in Fig. 3 . The values of the energy flux are normalized by .


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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Mode recombination and alternation of surface plasmons in anisotropic mediums