Diffractive Optical Element

last updated 2026-08-31

Physics / mechanism

A diffractive optical element (DOE) is a passive, typically static component that imposes a designed phase (and sometimes amplitude) profile on an incident beam, so that interference in the propagated field produces a target intensity distribution. Because the function is encoded in surface relief or a multilevel phase mask rather than in bulk refraction, one thin element can replace a train of lenses, beamsplitters and apertures. The most common use is beam splitting and beam shaping: converting a single Gaussian input into an array of foci, or into a structured probe with properties unattainable by focusing alone.

Multi-spot generation is the workhorse mode. A DOE can transform a Gaussian beam into a 2x2 array of co-propagating spots, which in laser-induced breakdown spectroscopy produces multiple ablation plumes that expand simultaneously and interact. The same principle extends into the third dimension: a single static DOE can be designed to place two independent focal-spot arrays in distinct axial planes, with 29 write spots split across two planes separated by 1.8 µm demonstrated for two-photon polymerization. Key design parameters are therefore the number and geometry of spots, the axial separation between planes, the uniformity of energy distribution, and the diffraction efficiency into the wanted orders.

Beyond replication of foci, multilevel DOEs can synthesise fields whose local structure beats the conventional focusing limit. In super-oscillatory label-free inertia-free scanning (SOLIS) microscopy, a static multilevel DOE generates compressed super-oscillatory probes, and a digital micromirror device selects among them so that scanning requires no stage motion; a 25-position scan yields one averaged map every 3.58 ms, or 279 reconstructed frames per second. On nanofabricated line-pair targets the approach retained measurable label-free contrast at a 253 nm period and resolved modulation at 270 nm.

The practical trade-off is that a static DOE fixes its function at fabrication time. Throughput gains come from parallelism rather than from reconfigurability: dual-plane multi-spot 2PP achieved an effective writing speed of 1 mm² in 90 s for four-layer woodpile structures while retaining a simple scanning strategy.

Competitive landscape

DOEs sit between fully refractive multi-beam optics and actively addressed modulators. Conventional multifocal systems built from bulk optics remain constrained by bulky architectures, stringent alignment requirements and susceptibility to laser-induced degradation under intense irradiation. Metasurfaces are the closest structural competitor: a monolithic diamond metalens with a 7.2 mm aperture and high-aspect-ratio truncated-cone nanopillars produced two focal spots separated by 200 µm at a 4 mm focal length, and under 25 W pulsed irradiation for 1 h showed a focal shift of only 25.5 µm. That points to material choice, not diffractive versus metasurface phase encoding, as the determinant of high-power survivability.

ApproachReconfigurableDemonstrated role in sources
Static DOENo2x2 beam splitting for LIBS; 29-spot dual-plane 2PP; super-oscillatory probes
DOE plus DMDProbe selection onlyInertia-free scanning without stage motion
Diamond metalensNoMultifocal high-power laser processing with thermal stability

Evidence base

Frontier (open questions)

Synthesised 2026-08-31 from 4 KB sources by the resynth pipeline; citations are KB source slugs.

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