2017
DOI: 10.1038/s41467-017-01515-2
|View full text |Cite
|
Sign up to set email alerts
|

Direct observation of valley-polarized topological edge states in designer surface plasmon crystals

Abstract: The extensive research of two-dimensional layered materials has revealed that valleys, as energy extrema in momentum space, could offer a new degree of freedom for carrying information. Based on this concept, researchers have predicted valley-Hall topological insulators that could support valley-polarized edge states at non-trivial domain walls. Recently, several kinds of photonic and sonic crystals have been proposed as classical counterparts of valley-Hall topological insulators. However, direct experimental… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1

Citation Types

5
287
3

Year Published

2017
2017
2023
2023

Publication Types

Select...
10

Relationship

0
10

Authors

Journals

citations
Cited by 345 publications
(298 citation statements)
references
References 57 publications
5
287
3
Order By: Relevance
“…According to k·p method, the effective Hamiltonian around K/K′ valley can be expressed as H K/K′ ( δ k ) = ±( v D δk x σ x + v D δk y σ y ) ± mv D 2 σ z , where δ k = k − k K/K′ is the displacement of wave vector k to K/K′ valley in the reciprocal space, v D is the group velocity, m is the effective mass term, and σ i = ( i = x, y, z ) are elements in the Pauli matrices . Solving the effective Hamiltonian, we can obtain the Berry curvature at K/K′ valley, ΩK/normalK(δk)=±mvnormalD2(δk2+m2vnormalD2)3/2 . In order to consolidate the above theoretical analysis, we calculate the Berry curvatures of the four bands near K valley by performing first‐principle simulations of the practical structure in the COMSOL Multiphysics, as shown in Figure e.…”
mentioning
confidence: 99%
“…According to k·p method, the effective Hamiltonian around K/K′ valley can be expressed as H K/K′ ( δ k ) = ±( v D δk x σ x + v D δk y σ y ) ± mv D 2 σ z , where δ k = k − k K/K′ is the displacement of wave vector k to K/K′ valley in the reciprocal space, v D is the group velocity, m is the effective mass term, and σ i = ( i = x, y, z ) are elements in the Pauli matrices . Solving the effective Hamiltonian, we can obtain the Berry curvature at K/K′ valley, ΩK/normalK(δk)=±mvnormalD2(δk2+m2vnormalD2)3/2 . In order to consolidate the above theoretical analysis, we calculate the Berry curvatures of the four bands near K valley by performing first‐principle simulations of the practical structure in the COMSOL Multiphysics, as shown in Figure e.…”
mentioning
confidence: 99%
“…Due to the high efficiency of the coupling between the topological modes and free space modes, we anticipate many practical applications for directional antennas, lasers, and other communication devices across the electromagnetic spectrum. During preparation of this work, two related reports 29,30 of experimental realizations of photonic valley edge states were brought to our attention. The fundamental difference of our work is the demonstration of topologically protected refraction.…”
mentioning
confidence: 99%
“…This map proves that the wave is indeed guided by the interface line between the two inverted dual‐metasurfaces with good localization and negligible scattering losses at the bends. Note that the edge modes are also robust against 90° bends, as demonstrated in Figure d, since they could also occur along the armchair edge of the hexagonal metasurface, unlike the so‐called valley topological insulators …”
Section: Resultsmentioning
confidence: 96%