2016
DOI: 10.1103/physrevlett.116.163901
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Topological Optical Waveguiding in Silicon and the Transition between Topological and Trivial Defect States

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Cited by 249 publications
(114 citation statements)
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“…Here, W is equivalent to the Zak phase, up to a factor of π. The winding number can be calculated by W=iπnormalkdkfalse⟨ψ(k)false|kfalse|ψ(k)false⟩ (where |ψfalse(kfalse) is Bloch wave functions), which takes on the value of 0 when c 1 > c 2 and 1 when c 1 < c 2 . Non‐zero winding number implies nontrivial topology and indicates the existence of edge states.…”
Section: Resultsmentioning
confidence: 99%
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“…Here, W is equivalent to the Zak phase, up to a factor of π. The winding number can be calculated by W=iπnormalkdkfalse⟨ψ(k)false|kfalse|ψ(k)false⟩ (where |ψfalse(kfalse) is Bloch wave functions), which takes on the value of 0 when c 1 > c 2 and 1 when c 1 < c 2 . Non‐zero winding number implies nontrivial topology and indicates the existence of edge states.…”
Section: Resultsmentioning
confidence: 99%
“…There are also 1D topological systems that have edge states that exist at the termination of a 1D lattice. For example, zero modes in the Su–Schriffer–Heeger (SSH) model have gained significant attention and have been explored in many different systems . All the progress in fundamental researches of topological photonics has recently prompted great efforts to design robust optical devices that are insensitive to structural perturbations and fabrication disorders.…”
Section: Introductionmentioning
confidence: 99%
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“…In the latter case, α m denotes electric field amplitude in m th cavity. Such correspondence allows one to investigate the physics of the SSH model in fully classical setups, including electronic [11,12], photonic [13][14][15][16][17][18][19], plasmonic [20][21][22][23], polaritonic [24] and mechanical [25] systems. The bulk energy spectrum of the SSH model is found from Eqs.…”
Section: Topological States In the Linear Ssh Modelmentioning
confidence: 99%
“…Possibly the simplest model of the topological states in one-dimensional systems is provided by the wellcelebrated Su-Schrieffer-Heeger model (SSH) [11,12], which was investigated and realized in various contexts including electronic [11,12], photonic [13][14][15][16][17][18][19], plasmonic [20][21][22][23], polaritonic [24] and mechanical [25] systems. Though initially the SSH model was applied to explain charge transfer in polymer molecules, it can be also used for describing the physics of artificial photonic and plasmonic structures.…”
Section: Introductionmentioning
confidence: 99%