2020
DOI: 10.1109/tap.2020.2969725
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Non-Reciprocal, Robust Surface Plasmon Polaritons on Gyrotropic Interfaces

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Cited by 33 publications
(12 citation statements)
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“…Then, as in the case of quantum-Hall topological insulators in condensed-matter physics [21], topologically-protected unidirectional surface waves may emerge when an interface is formed with a material having a bulk-mode bandgap with different topological properties (the opaque isotropic material in our case) [4,7]. Conversely, the first type of SPPs discussed above, which exist on an interface with a transparent medium, are not topologically-protected, as the lower bulkmode bandgap is topologically trivial [9].…”
Section: Nonreciprocal Plasmonic Platformsmentioning
confidence: 97%
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“…Then, as in the case of quantum-Hall topological insulators in condensed-matter physics [21], topologically-protected unidirectional surface waves may emerge when an interface is formed with a material having a bulk-mode bandgap with different topological properties (the opaque isotropic material in our case) [4,7]. Conversely, the first type of SPPs discussed above, which exist on an interface with a transparent medium, are not topologically-protected, as the lower bulkmode bandgap is topologically trivial [9].…”
Section: Nonreciprocal Plasmonic Platformsmentioning
confidence: 97%
“…It has been known for several decades that, at the interface between a magnetized plasma (a gyrotropic medium) and an isotropic material, unidirectional surface waves can emerge under certain conditions and in certain frequency ranges (e.g., [1][2][3]). This topic has seen a recent resurgence of interest in the context of nonreciprocal and topological electromagnetics [4][5][6][7][8][9][10][11][12][13][14][15][16]. Particularly intriguing is the possibility of realizing truly unidirectional wave-propagation channels, combined with the high degree of field localization and confinement of plasmonic platforms, which may enable extreme and counter-intuitive optical effects, especially if the one-way channel is abruptly terminated or closed.…”
Section: Introductionmentioning
confidence: 99%
“…This regime has been studied in detail in Refs. [33][34][35]. If the bias is turned off, ω c = 0, the system becomes reciprocal, the two Weyl points annihilate each other at k z = 0, and the Weyl material undergoes a topological phase transition to a trivial state.…”
Section: Nonreciprocal Implementationmentioning
confidence: 99%
“…As the frequency approaches the unidirectional window described previously, the equifrequency contours become more elliptical and the SPP modes propagate with stronger anisotropy. Finally, within the unidirectional window, we see from Figure 5b that the equifrequency contours become open and no backward-propagating mode exist in the −x direction, at least in the local case [58] (in the nonlocal case, the equifrequency contours close for very large values of wavevector). Furthermore, due to the hyperbolic-like shape of the equifrequency contours, a point source near the surface would launch SPPs propagating as narrow diffraction-less beams [59].…”
Section: Surface States-transparent Opaque and Other Interfacesmentioning
confidence: 82%