OSA Nonlinear Optics 2021 2021
DOI: 10.1364/nlo.2021.nm2a.6
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Localized light in a fractal-like photonic lattice

Abstract: We demonstrate light localization in a frustrated fractal-like photonic lattice owing multiple flat bands fabricated by femtosecond direct laser writing. We investigate the arising flat bands depending on the singularities of their Bloch wave functions.

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Cited by 1 publication
(2 citation statements)
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“…Such a DHL (also called “star lattice” [ 2,4,5 ] ) is different from previous HCL variations such as the super HCLs [ 37 ] that consist of five lattice sites per unit cell and host only a single flat band, although the term “decorated HCL” was somewhat mix‐used in literature. [ 40,41 ] The DHL considered here is also different from the fractal‐like lattices, [ 32,33 ] which also have six lattice sites per unit cell but only with one singular flatband touching. A light beam propagating in a photonic DHL is described by the Schrödinger‐like paraxial wave equation [ 42,43 ] izΨfalse(x,y,zfalse)=(badbreak−12k2goodbreak−kΔnfalse(x,yfalse)n0)Ψfalse(x,y,zfalse)=H0Ψfalse(x,y,zfalse)\[i{\partial _z}{\bm{\Psi }}(x,y,z) = \left( { - \frac{1}{{2k}}\nabla _ \bot ^2 - \frac{{k\Delta n(x,y)}}{{{n_0}}}} \right){\bm{\Psi }}(x,y,z) = {H_0}{\bm{\Psi }}(x,y,z)\] where Ψ ( x , y , z ) is the envelope of the electric field, k is the wavenumber, Δ n is the induced refractive index change that forms a DHL potential, n 0 is the bulk refractive index, and H 0 is the Hamiltonian operator.…”
Section: Construction Of Dhl and Theoretical Analysis Of Singular Fla...mentioning
confidence: 99%
See 1 more Smart Citation
“…Such a DHL (also called “star lattice” [ 2,4,5 ] ) is different from previous HCL variations such as the super HCLs [ 37 ] that consist of five lattice sites per unit cell and host only a single flat band, although the term “decorated HCL” was somewhat mix‐used in literature. [ 40,41 ] The DHL considered here is also different from the fractal‐like lattices, [ 32,33 ] which also have six lattice sites per unit cell but only with one singular flatband touching. A light beam propagating in a photonic DHL is described by the Schrödinger‐like paraxial wave equation [ 42,43 ] izΨfalse(x,y,zfalse)=(badbreak−12k2goodbreak−kΔnfalse(x,yfalse)n0)Ψfalse(x,y,zfalse)=H0Ψfalse(x,y,zfalse)\[i{\partial _z}{\bm{\Psi }}(x,y,z) = \left( { - \frac{1}{{2k}}\nabla _ \bot ^2 - \frac{{k\Delta n(x,y)}}{{{n_0}}}} \right){\bm{\Psi }}(x,y,z) = {H_0}{\bm{\Psi }}(x,y,z)\] where Ψ ( x , y , z ) is the envelope of the electric field, k is the wavenumber, Δ n is the induced refractive index change that forms a DHL potential, n 0 is the bulk refractive index, and H 0 is the Hamiltonian operator.…”
Section: Construction Of Dhl and Theoretical Analysis Of Singular Fla...mentioning
confidence: 99%
“…[ 11 ] Flatband systems have attracted considerable attention over the decades, for instance, in the study of Anderson localization, [ 12,13 ] bosonic condensation [ 14 ] and fractional quantum Hall states, [ 15,16 ] and have been realized in a variety of synthetic platforms recently, [ 11 ] including engineered electronic lattices, [ 17–19 ] optical lattices for cold atoms, [ 20 ] polaritonic lattices [ 21 ] and photonic lattices. [ 22–28 ] In particular, an extensively studied phenomenon using photonic lattices is the formation of compact localized states (CLSs), [ 29,30 ] realized with a variety of flatband lattice geometry such as Lieb, [ 22,23 ] Kagome, [ 25 ] rhombic, [ 31 ] and fractal‐like [ 32–34 ] lattices.…”
Section: Introductionmentioning
confidence: 99%