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Can a metasurface sort light by twist and colour at once?

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A single silicon metasurface can store ten separate images, shown only when it is lit with the right colour and the right amount of optical twist (orbital angular momentum).

Source

Multiplexed manipulation of orbital angular momentum and wavelength in metasurfaces based on arbitrary complex-amplitude control

He G, Zheng Y, Zhou C, et al. · Light, science & applications · 2024

doi.org/10.1038/s41377-024-01420-6Read the full paper ↗29 citationscc by

Study at a glance

Design
Other — FDTD-optimised crystalline-silicon nanopillar 'multiplexed coherent pixels', fabricated as a 1200 x 1200 metasurface and tested with plane and OAM beams at 473 and 633 nm
N
No sample size; one main fabricated metasurface plus an OAM demultiplexer demonstration
Population
Crystalline silicon nanopillar metasurfaces on fused silica
Outcome
Reconstructed printing images and OAM-selective holograms, crosstalk, and optical efficiency

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What they did

The authors built pixels from pairs of identical silicon nanopillars whose rotation-angle difference sets the amplitude and whose mean angle sets the phase for circularly polarized light. Two pillar lengths were tuned to respond to blue (473 nm) and red (633 nm) light with little crosstalk. Holograms were encoded with spiral phases and a sampling array so each responds only to a matching OAM topological charge, combined with printed images using a modified Gerchberg-Saxton algorithm, then fabricated and imaged.

What they found

Plane waves displayed a binary smiley face in blue and a grayscale star in red at the metasurface with almost no crosstalk, while OAM beams with charges of -6, -3, 3 and 6 reconstructed eight different letters at wavelength-specific distances. Measured efficiency was about 5.4 percent against about 23 percent in theory. The design packed ten channels into a 0.64 square-micron pixel, roughly halving the area per channel compared with an earlier benchmark, and also worked as an OAM demultiplexer routing different charges and colours to different spots.

The limits

What it doesn't show

Experimental efficiency was low and well below theory, which the authors attribute to deliberately reduced amplitudes, fabrication errors and losses in polarizers and wave plates. Hologram quality degraded when adjacent topological charges were closer together (spacing of 1 instead of 3), so the number of usable OAM channels is limited by crosstalk. The demultiplexer was only demonstrated for two topological charges because of experimental constraints, and holograms are digitised by the sampling array.

Key terms

Orbital angular momentum (OAM)
A property of light with a helical wavefront, described by an integer topological charge l that counts the phase twists around the beam axis.
Topological charge
The integer l giving how many multiples of 2 pi the phase winds around an OAM beam's axis.
Coherent pixel
A metasurface unit of identical nanopillars whose combined output sets both amplitude and phase through their rotation angles.
Pancharatnam-Berry phase
A geometric phase of twice the rotation angle given to cross-polarized circular light by a rotated anisotropic pillar.
Demultiplexer
A device that separates combined signal channels, here different OAM modes and wavelengths, to different output positions.

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Quiz yourself

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What sets the amplitude in a coherent pixel?

Common questions

How does a pair of rotated pillars control amplitude?

Each pillar adds a phase of twice its angle; summing the two outputs gives an amplitude set by the cosine of their angle difference and a phase set by their average angle.

Why does each hologram respond only to one OAM beam?

The hologram carries a spiral phase opposite to one topological charge, so only that incoming beam is flattened into a focused signal that passes the sampling-array filter.

Why were charges spaced by three?

Closer charges like -2, -1, 1, 2 overlapped in momentum space and caused crosstalk that degraded the images.

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