2022
DOI: 10.1002/adom.202102523
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Localized States Emerging from Singular and Nonsingular Flat Bands in a Frustrated Fractal‐Like Photonic Lattice

Abstract: Singular and nonsingular flat bands in a Sierpinski fractal‐like photonic lattice are reported. It is demonstrated that the lowest two bands, being isolated and degenerate due to geometrical frustration, are nonsingular and thus can be spanned by a complete set of compact localized states. These states are experimentally proven to propagate diffractionless in the photonic lattice. The results reveal the interplay between geometrical frustration, degenerate flat bands, and compact localized states in a single p… Show more

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Cited by 14 publications
(18 citation statements)
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References 48 publications
(67 reference statements)
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“…The distribution is preserved even if the finite size of the gasket is arbitrarily large. Interestingly, almost exact replicas of the amplitude patterns discussed above, have been experimentally observed recently in photonic lattices 26,27 where, a variant of the SGF structure reported here has been studied in two dimensions. In spite of the variation in construction, the ring-like CLS and the armchair patterns described here in Fig.…”
Section: The Sierpinski Gasket: Engineering Compact Localization and ...supporting
confidence: 61%
See 1 more Smart Citation
“…The distribution is preserved even if the finite size of the gasket is arbitrarily large. Interestingly, almost exact replicas of the amplitude patterns discussed above, have been experimentally observed recently in photonic lattices 26,27 where, a variant of the SGF structure reported here has been studied in two dimensions. In spite of the variation in construction, the ring-like CLS and the armchair patterns described here in Fig.…”
Section: The Sierpinski Gasket: Engineering Compact Localization and ...supporting
confidence: 61%
“…This works easily when the unit cell has simple geometry, but turns out to be a tedious job in cases where the unit cell has an intricate internal structure. This issue has become pertinent and needs to be addressed, in particular, after a series of fascinating experiments reported laboratory realizations of the classic Sierpinski gasket fractal (SGF) [23][24][25] and observation of CLS [26][27][28][29][30] and photonic Floquet topological phase 31 on engineered SGF substrates. The latter experiments were done on SGF structures grafted either mainly by the femtosecond laser writing techniques, or designed with evanescently coupled helical waveguides, for example.…”
Section: Introductionmentioning
confidence: 99%
“…Since the CLS‐2 and CLS‐3 share the same eigenvalue (propagation constant), their superimposed states (CLS‐5 and CLS‐6) are also eigenstates of the plane‐touching flat bands. [ 18,19 ] Thus, for the doubly‐degenerate flat bands β 5, 6 , there exist two different sets of basic CLSs, one set consists of {CLS‐2} and {CLS‐3}, the other one consists of {CLS‐5} and {CLS‐6}, where the notation “false{·false}$\{\cdot \}$” indicates N translated copies of the selected basic CLS. When we choose one of the sets, {CLS‐2, CLS‐3} for example, {CLS‐2} corresponds to the flat band β 5 , then {CLS‐3} automatically corresponds to flat band β 6 , and vice versa.…”
Section: Resultsmentioning
confidence: 99%
“…In order to verify our results experimentally, we fabricated photonic lattices in fused silica (SiO 2 ) using the direct laser writing technique [24,40]. Table II shows the main differences in parameters compared to the simulations presented so far.…”
Section: Experiments In Fused Silicamentioning
confidence: 87%