2019
DOI: 10.1103/physrevb.99.245414
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Unidirectional and diffractionless surface plasmon polaritons on three-dimensional nonreciprocal plasmonic platforms

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Cited by 46 publications
(13 citation statements)
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“…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%
“…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%
“…They may enable multiple striking topological features such as Majorana type edge states and zero mode 22 , which do not exist in inversion symmetry breaking systems. Although there have been theoretical proposals on implementation of Weyl degeneracies by applying external magnetic fields on finely designed photonic crystals 16,31 , very few of them are easily realizable in experiment due to the challenge in three-dimensional structuring of magnetic materials 32,33 . Interestingly, it was recently theoretically proposed that plasma, the fourth fundamental state of natural matter 34,35 , can support Weyl degeneracies under external magnetic fields 19 , as well as nonreciprocal wave transport [36][37][38] . Since there is no structuring involved, this represents a facile and tunable approach for achieving photonic Weyl degeneracies arising from time-reversal symmetry breaking.…”
Section: Photonic Weyl Points Due To Broken Time-reversal Symmetry Inmentioning
confidence: 99%
“…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]. This is because the asymptotic part of the equifrequency contours tend to dominate the response, resulting in highly collimated energy flow (group velocity vectors are normal to the equifrequency contour), as shown in Figure 5c.…”
Section: Surface States-transparent Opaque and Other Interfacesmentioning
confidence: 99%
“…For additional details on this interesting behavior, analogous to diffractionless wave propagation in hyperbolic metamaterials, but with the additional benefit of quasi-unidirectionality, we refer the interested readers to Ref. [59].…”
Section: Surface States-transparent Opaque and Other Interfacesmentioning
confidence: 99%