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Multiplying and dividing the twist of a light beam

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A pair of patterned optical surfaces on a single glass chip can double or triple the orbital angular momentum of a light beam, or split it into beams carrying a half or a third of it.

Source

Multiplication and division of the orbital angular momentum of light with diffractive transformation optics

Ruffato G, Massari M, Romanato F · Light, science & applications · 2019

doi.org/10.1038/s41377-019-0222-2Read the full paper ↗24 citationscc by

Study at a glance

Design
Other — Theory and Fresnel simulations of circular-sector conformal transformations, followed by e-beam-lithography fabrication of diffractive multipliers/dividers and interferometric testing with SLM-generated OAM beams.
N
No sample; devices for twofold and threefold multiplication and division were each tested over a range of input OAM values.
Population
Laser beams (632.8 nm HeNe) carrying integer orbital angular momentum
Outcome
Output OAM value (counted from spiral interferogram arms) and beam intensity profiles

Structured fields used in claim comparison tables when every cited study has a complete layer.

What they did

The authors derived phase patterns for an optical transformation that maps a full circle onto a circular sector, and superposed several such transformations to multiply or divide a beam's azimuthal phase gradient. They simulated the beam propagation, then fabricated the transformer and its phase corrector side-by-side on a single substrate using electron-beam lithography, with a mirror folding the beam back onto the corrector. They tested the devices with OAM beams from a spatial light modulator and read the output OAM from the spiral arms in interferograms.

What they found

The twofold multiplier doubled input OAM values from −4 to +4 and the threefold multiplier tripled values from −3 to +3, as shown by the number of spiral arms. The twofold divider split beams with even OAM from −8 to +8 into two beams each carrying half the OAM, and the threefold divider split inputs from −9 to +9 into three beams each carrying a third. Simulations indicated conversion efficiency close to perfect, dropping slowly at higher input OAM because the beam's twisted wavefront distorts the output ring.

The limits

What it doesn't show

Only twofold and threefold operations and modest OAM values were demonstrated experimentally; performance at high OAM or in cascades is proposed, not shown. The paper reports efficiency mainly from simulation rather than a measured experimental efficiency, and outputs show slight asymmetric distortion. Division here produces equal output modes only, and applications like OAM computing or single-photon use are speculative.

Key terms

Orbital angular momentum (OAM) of light
Angular momentum carried by a beam with a helical phase front exp(iℓθ); ℓ counts the phase twists per turn.
Conformal optical transformation
A mapping of beam coordinates, implemented by a phase element plus a corrector, that reshapes the beam while preserving local angles.
Phase corrector
The second optical element that removes the phase distortion accumulated by the transformed beam and restores the intended phase profile.
Spiral interferogram
The pattern made by interfering an OAM beam with a reference beam; the number of spiral arms reveals ℓ.
Electron-beam lithography
A fabrication technique that writes nanometre-scale patterns into a resist by controlled electron dose, here producing multilevel surface-relief optics.

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Quiz yourself

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What does the integer ℓ describe for an OAM beam?

Common questions

Why is multiplying OAM harder than adding to it?

Standard elements like spiral phase plates just add a fixed azimuthal phase; multiplying requires rescaling the existing phase gradient, which needs a coordinate transformation of the beam.

How was the output OAM measured?

By interfering the output with a reference beam in a Mach-Zehnder setup and counting the spiral arms in the resulting pattern.

Why put both elements on one substrate?

It makes them automatically parallel and aligned, reducing the hard alignment problem of two separate confocal elements and aiding miniaturisation.

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