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Can one nano-hole respond to twist one way and angle the other?

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A tiny helix-shaped hole in gold lets through one handedness of circularly polarised light from the front, but from the back it instead filters by linear polarisation angle, allowing two hidden images in one chip.

Source

3D Janus plasmonic helical nanoapertures for polarization-encrypted data storage

Chen Y, Yang X, Gao J · Light, science & applications · 2019

doi.org/10.1038/s41377-019-0156-8Read the full paper ↗81 citationscc by

Study at a glance

Design
Other — Finite-element simulation plus focused-ion-beam fabrication and polarisation-resolved transmission measurements of helical nanoaperture arrays in gold, lit from front and back, then a Janus metasurface encoding two images.
N
No participant sample; results come from simulated unit cells and fabricated nanoaperture arrays, including one encoded metasurface built from 31 × 31 squares of 7 × 7 unit cells.
Population
Helical nanoapertures milled in a gold film on silica, in both mirror-image forms
Outcome
Forward circular dichroism in transmission, backward linear dichroism in transmission, and readability of the encoded QR-code and greyscale images

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What they did

The authors designed a helical nanoaperture: an arc-shaped hole joined to a groove whose depth ramps from zero to right through a 180 nm gold film, milled in one step with grayscale focused-ion-beam milling. They simulated and measured how much light passed for left- and right-handed circular polarisation from the front and for different linear polarisation angles from the back. They then built a metasurface where the choice of mirror-image form set a QR-code pixel and the rotation angle of each aperture set a greyscale pixel via Malus's law.

What they found

From the front, the measured circular dichroism in transmission peaked at 0.72 at 830 nm and exceeded 0.5 over roughly 680 to 900 nm, close to simulations. The effect came mainly from handedness-dependent reflection caused by mode coupling along the ramped groove, not from absorption, which is why a film thinner than a quarter wavelength sufficed. From the back, circular dichroism vanished, as reciprocity predicts, but linear dichroism reached up to about 0.87. The encoded chip showed a scannable QR code only under right-handed light from the front and a Bohr portrait only under x-polarised light from the back, with a working band of approximately 200 nm.

The limits

What it doesn't show

Measured and simulated spectra differ somewhat, which the authors attribute to ion-beam fabrication tolerance, gold film quality and optical component imperfections. The paper reports two slightly different peak linear dichroism values (0.87 and 0.88) for the backward direction. Serial ion-beam milling took hours for one small metasurface, so it does not show a scalable manufacturing route, and the demonstration is limited to near-infrared wavelengths within a finite resonant band.

Key terms

Chirality
A shape that cannot be superimposed on its mirror image, like left and right hands; its two versions are enantiomers.
Circular dichroism in transmission
The normalised difference between how much right- and left-handed circularly polarised light passes through a structure.
Linear dichroism
The normalised difference in transmission between two perpendicular linear polarisations.
Lorentz reciprocity
A symmetry of linear optics linking transmission in one direction to transmission in the reverse direction, which here fixes how the Jones matrix changes when the sample is flipped.
Malus's law
Transmitted intensity through a polariser varies as the squared cosine of the angle between light polarisation and the transmission axis.
Grayscale focused-ion-beam milling
Ion-beam etching where the local dose is varied so that depth changes continuously, allowing ramps and 3D profiles in one step.

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What does the helical nanoaperture do for light arriving from the front?

Common questions

Why is the circular dichroism not caused mainly by absorption?

The authors' reflection and absorption spectra show that the transmission difference comes mostly from handedness-dependent reflection, because light couples more efficiently between the successive arc-shaped segments for one handedness.

Why does the circular dichroism disappear when light comes from the back?

Reciprocity swaps and sign-flips the cross-polarised terms; because the aperture's front-side output is linearly polarised, reversing the direction turns it into a linear polariser that accepts both handedness components equally.

How can two images be stored without interfering?

Choosing the mirror-image form of each aperture sets its forward circular response, while rotating it sets its backward linear response, and each choice barely affects the other.

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