Moiré lattices consist of two superimposed identical periodic structures with a relative rotation angle. Moiré lattices have several applications in everyday life, including artistic design, the textile industry, architecture, image processing, metrology and interferometry. For scientific studies, they have been produced using coupled graphene–hexagonal boron nitride monolayers1,2, graphene–graphene layers3,4 and graphene quasicrystals on a silicon carbide surface5. The recent surge of interest in moiré lattices arises from the possibility of exploring many salient physical phenomena in such systems; examples include commensurable–incommensurable transitions and topological defects2, the emergence of insulating states owing to band flattening3,6, unconventional superconductivity4 controlled by the rotation angle7,8, the quantum Hall effect9, the realization of non-Abelian gauge potentials10 and the appearance of quasicrystals at special rotation angles11. A fundamental question that remains unexplored concerns the evolution of waves in the potentials defined by moiré lattices. Here we experimentally create two-dimensional photonic moiré lattices, which—unlike their material counterparts—have readily controllable parameters and symmetry, allowing us to explore transitions between structures with fundamentally different geometries (periodic, general aperiodic and quasicrystal). We observe localization of light in deterministic linear lattices that is based on flat-band physics6, in contrast to previous schemes based on light diffusion in optical quasicrystals12, where disorder is required13 for the onset of Anderson localization14 (that is, wave localization in random media). Using commensurable and incommensurable moiré patterns, we experimentally demonstrate the two-dimensional localization–delocalization transition of light. Moiré lattices may feature an almost arbitrary geometry that is consistent with the crystallographic symmetry groups of the sublattices, and therefore afford a powerful tool for controlling the properties of light patterns and exploring the physics of periodic–aperiodic phase transitions and two-dimensional wavepacket phenomena relevant to several areas of science, including optics, acoustics, condensed matter and atomic physics.
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The data that support the findings of this study are available from the corresponding author upon reasonable request.
The codes that support the findings of this study are available from the corresponding author upon reasonable request.
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P.W. and F.Y. acknowledge support from the NSFC (grant numbers 91950120, 11690033 and 61475101). Y.V.K. and L.T. acknowledge support from the Severo Ochoa Excellence Programme (SEV-2015-0522), Fundacio Privada Cellex, Fundacio Privada Mir-Puig and CERCA/Generalitat de Catalunya. F.Y. thanks Z. Chen, Y. Hu and D. Song for technical discussions on the experiment with the SBN crystals.
The authors declare no competing interests.
Publisher’s note Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Extended data figures and tables
Experimentally observed intensity distributions of the probe beam (colour-surface plots) and corresponding theoretically calculated distributions (insets) at different propagation distances z, for tanθ = 3−1/2 and p2 = 0.1 (below the LDT point; top row), tanθ = 3−1/2 and p2 = 1 (above the LDT point; middle row) and tanθ = 3/4 and p2 = 1 (bottom row). The two top rows correspond to the incommensurable Pythagorean lattice shown in Fig. 1b. The third row corresponds to the commensurable lattice shown in Fig. 1c.
Extended Data Fig. 2 Numerical simulation of light propagation to distances beyond the crystal length.
a, b, Numerical simulations of the light-beam propagation in the incommensurable moiré lattice for central excitation, corresponding to the top and middle rows of Extended Data Fig. 1, but for larger distances, exceeding the sample length. c, d, Similar numerical results, but for an off-centre excitation position in the moiré lattice. p2 = 0.1 (a, c), p2 = 1.0 (b, d), θ = π/6. In all cases, a Gaussian beam exciting a single site of the potential is assumed.
λ/2, half-wave plate; PBS, polarizing beam splitter; SF, spatial filter; L, lens; BS, beam splitter; ID, iris diaphragm; M, mirror; P, polarizer; SBN, strontium barium niobate crystal; CCD, charged-coupled device. Mask 2 is an amplitude mask used to produce two group of sub-lattices with rotation angle θ, and mask 1 is made of a polarizer film.
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Wang, P., Zheng, Y., Chen, X. et al. Localization and delocalization of light in photonic moiré lattices. Nature 577, 42–46 (2020) doi:10.1038/s41586-019-1851-6