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. 2019 Oct 21;10(1):4789.
doi: 10.1038/s41467-019-12637-0.

Dielectric multi-momentum meta-transformer in the visible

Affiliations

Dielectric multi-momentum meta-transformer in the visible

Lei Jin et al. Nat Commun. .

Abstract

Metasurfaces as artificially nanostructured interfaces hold significant potential for multi-functionality, which may play a pivotal role in the next-generation compact nano-devices. The majority of multi-tasked metasurfaces encode or encrypt multi-information either into the carefully tailored metasurfaces or in pre-set complex incident beam arrays. Here, we propose and demonstrate a multi-momentum transformation metasurface (i.e., meta-transformer), by fully synergizing intrinsic properties of light, e.g., orbital angular momentum (OAM) and linear momentum (LM), with a fixed phase profile imparted by a metasurface. The OAM meta-transformer reconstructs different topologically charged beams into on-axis distinct patterns in the same plane. The LM meta-transformer converts red, green and blue illuminations to the on-axis images of "R", "G" and "B" as well as vivid color holograms, respectively. Thanks to the infinite states of light-metasurface phase combinations, such ultra-compact meta-transformer has potential in information storage, nanophotonics, optical integration and optical encryption.

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Conflict of interest statement

The authors declare no competing interests.

Figures

Fig. 1
Fig. 1
Comparative elaborations of multi-tasked metasurfaces (ac) and our multi-momentum meta-transformer (dh). a Schematic illustration of a spatially multiplexed metasurface. The spatial multiplexed metasurface reconstructed several distinguished field distribution U(n) based on the spatial separations of metasurface S0(n) or observed region (S(n)). The x0 and y0 (x, y, and z) are the coordinated variables of the metasurface plane S0 (observation region S). b Illustration of a structurally multiplexed metasurface–,,. The structurally multiplexed metasurface reconstructed several distinguished field distribution U(n) based on the metasurface function Umeta(n). c Schematic illustration of a multi-beam meta-opener. The multi-beam meta-opener is formed by several kinds of “key arrays”, which is used to read out the distributions U(n) carried by the preset incident beams. d Illustration of transmission-type multi-momentum meta-transformer. The multi-momentum meta-transformer decoder phase profile is implemented with TiO2 nano-fin array with in-plane orientations on a quartz substrate. It controls multi-beams with different momenta (l(nand k0n) to reconstruct corresponding field distributions U(n) Schematic of the OAM meta-transformer. Under the illumination of vortex beams with right circular polarization (RCP), the decoder can generate distinct images at the same plane with left circular polarization (LCP). f Schematic of the LM meta-transformer. Under the illumination of different LM beams with RCP, the meta-transformer can generate distinct LM-dependent field distributions at the same region on optical axis. g Top-view scanning electron microscopy (SEM) images of a partial region of the fabricated TiO2 nano-fins arrays. Scale bar: 2 μm. h Oblique-view SEM image. Scale bar: 2 μm. Each TiO2 nano-fin represents a phase pixel as defined in the meta-transformer
Fig. 2
Fig. 2
Principle and demonstration of multi-momentum meta-transformer. a Geometry of the designed unit cell structure representing one pixel in the meta-transformer, with the periodicity of 325 nm. The TiO2 nano-fin parameters are w = 80 nm, l = 250 nm, and h = 600 nm. The in-plane rotating angle φ of nano-fin will introduce the geometric phase of 2φ for the incident beam with RCP. b Measured conversion efficiency of the meta-transformer. The conversion efficiency is defined as the optical power of the transmitted light with opposite CP divided by the incident optical power. c Design principle of OAM meta-transformer. Under the illumination of vortex beam 1 (l(1) = −5) with RCP, the transmitted beam with opposite CP carries the total phase profile ψOAM=5x0,y0+ψmetax0,y0 and reconstructs “apple” pattern in the observation plane. When using vortex beam 2 (l(2) = 5) with RCP, the total phase profile of the transmitted beam is ψOAM=5x0,y0+ψmetax0,y0, which causes the reconstructed pattern change to a spider-shaped pattern. d Simulated (top) and measured (bottom) reconstructed patterns by vortex beam 1 (l(1) = −5) (left) and vortex beam 2 (l(2) = 5) (right). Scale bar: 20 μm. e Design principle of LM meta-transformer. Under the illumination of right circularly polarized beam with LM=k0Rħ, the transmitted beam with opposite CP carry the dispersionless phase profile of metasurface ψmeta (x0, y0). Due to the convolution of Uincx0,y0expiψmetax0,y0 and impulse response hx,y,z,k0R, the transmitted beam reconstructs patterns at the observation plane. Because the impulse response is k0-dependent, by changing LM of incidence, the reconstructed images “R”, “G” and “B” components can be shifted to one identical plane (z = Z0). f Simulated (top) and experimental (bottom) reconstruction of three-primary color holograms at the imaging plane. Scale bar: 20 μm. The original “spider” image was obtained from PNG image website
Fig. 3
Fig. 3
OAM meta-transformer for the read-out of three OAM states. a Schematic of OAM meta-transformer designed on three OAM states. This meta-transformer is designed to reconstructed “0”, “3” and “6” patterns at l(n) = 0, 3, and 6, respectively. b Simulated (top) and measured (bottom) reconstructed patterns. Scale bar: 20 μm
Fig. 4
Fig. 4
Reconstruction of color images. a Schematic illustration of reconstruction of gradient color image. b Intensity profiles corresponding to red, green, and blue beams and the graded color holographic image. Scale bar: 30 μm. The original “merlion” image was obtained from Vecteezy.com

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