Metasurface Lens
Replace a curved chunk of glass with a flat sheet of nano-pillars — and focus light just as sharply.
Replaces the smooth curved surface of a refractive lens with a subwavelength array of nanostructures (typically TiO₂, silicon, or GaN pillars on glass) that imposes a custom phase profile on the transmitted light. Choosing pillar height, width, and orientation locally produces any desired phase profile, including the hyperbolic profile required for diffraction-limited focusing. A single TiO₂ metalens can reach NA = 0.85 with >86% transmission at visible wavelengths and image quality comparable to commercial objectives.
Each nanopillar is a truncated waveguide: light passing through accumulates a phase delay determined by the pillar's effective refractive index and geometry. For TiO₂ (n ~ 2.3–2.5 at 532 nm), pillars about 600 nm tall with diameters from ~100 to ~350 nm cover a 0–2π phase range with high transmission. The metalens designer assigns each unit cell — a square lattice of pitch ~250–425 nm — the pillar geometry that contributes the right phase to bend light toward the focal point. For a lens of focal length f, the phase profile is φ(x,y) = −(2π/λ)(√(x² + y² + f²) − f). Achromatic metalenses balance phase and group delay across pillar libraries to reduce chromatic aberration. Fabrication uses atomic-layer-deposition TiO₂ into electron-beam-lithographed resist, followed by lift-off — yielding nearly vertical sidewalls and high aspect ratios.
In plain terms
A normal glass lens is thick and curved because it slows light down gradually as it enters, bending the beam smoothly. A metalens does the same job, but like a sheet of music: each tiny pillar on the surface is tuned to shift the incoming light wave by exactly the right amount, from zero up to one full wave. When all those tiny shifts add up, the light converges to a perfect focus. Because the lens is just a flat surface covered in nanoscale 'notes,' it can be a few micrometers thick — thinner than a red blood cell — yet work as precisely as a high-end microscope objective.
Also called: metalens, flat lens, dielectric metasurface optic.
Why it matters
- A metalens stack could replace 5–8 element lens stacks in smartphone cameras with a single flat element, dramatically thinning the module.
- Centimeter-scale DUV-manufactured metalenses point toward lighter AR/VR optics — millimeter-thick instead of centimeter-thick.
- Compact metalens-based spectrometers achieve nanometer-resolution dispersion in centimeter footprints — orders of magnitude smaller than grating spectrometers.
- Standard semiconductor lithography (e-beam or DUV) makes metalenses CMOS-foundry compatible.
Where it lives
- Capasso Group, Harvard SEAS — founding lab (2016 Science paper); achromatic and DUV-manufactured metalenses
- Metalenz, Inc. (Cambridge, MA) — semiconductor-foundry metalenses for sensors and consumer cameras
- Nano-optic endoscope (Harvard / Wellman Center) — metalens-based confocal imaging in bronchial airways
- IMEC / Samsung Advanced Institute — industrial integration with CMOS image sensors
Key numbers
- Lens thickness (TiO₂ metalens): 640 nm = 0.64 µm (~100× thinner than a human hair)
- NA (Capasso 2016): 0.85 (At 532 nm and 660 nm)
- Transmission efficiency: >60–86% (TiO₂ metalens at target wavelength)
- Mass-produced metalens aperture (DUV): 1–2 cm diameter
- Unit-cell pitch (subwavelength): 250–425 nm (Prevents grating lobes)
- Achromatic bandwidth: 490–550 nm (0.2 NA broadband design (Capasso group))
Surprising facts
- The Capasso group's 2016 metalens was about 600 µm in diameter and 640 nm thick — roughly 1,000× thinner than the glass substrate it sat on.
- A 1 cm metalens manufactured by deep-UV lithography contains roughly 10 billion nanopillars, comparable to the transistor count of a leading-edge processor — each pillar positioned with nanometer accuracy.
- A single flat metasurface can simultaneously act as a lens, a polarization analyzer, and a wavelength selector — replacing several bulky elements with one printed pattern.
- The TiO₂ pillars are taller than they are wide, with aspect ratios of 4–6 — closer in shape to redwood trees than to LEGO blocks.
Open questions
- Off-axis and broadband aberration trade-off: Single-layer metalenses suffer severe coma and field curvature for incidence angles beyond ~5–10°, far worse than conventional spherical lenses. Achromatic designs extend wavelength coverage but worsen field of view. The fundamental design trade-off between NA, bandwidth, and field of view is an open theoretical problem with no universal solution demonstrated.
A short history
The idea of a flat lens built from subwavelength resonant elements emerged from plasmonic-metasurface work in the early 2000s. In 2016, Khorasaninejad, Chen, Devlin, Zhu, and Capasso at Harvard published the TiO₂ dielectric metalens in Science, demonstrating diffraction-limited NA = 0.8 focusing at visible wavelengths. Achromatic metalenses followed in 2018 (Capasso group, Science). Centimeter-scale metalenses manufactured by deep-UV lithography arrived by 2022. Commercial development followed via the Metalenz spinoff. The 2017 Science review by Khorasaninejad and Capasso established field terminology and roadmap.
Sources
- Science (2016) — Khorasaninejad et al., TiO₂ metalens (https://www.science.org/doi/abs/10.1126/science.aaf6644)
- Science (2017) — Khorasaninejad & Capasso review (https://www.science.org/doi/10.1126/science.aam8100)
- Capasso Group Harvard — metasurfaces & flat optics (https://capasso.seas.harvard.edu/metasurfaces-and-flat-optics)
- Nature (2025) — review of optical metalens (https://www.nature.com/articles/s41378-025-01064-5)
- Stanford Fan Lab — Roadmap for Optical Metasurfaces (2024) (https://fanlab.stanford.edu/wp-content/papercite-data/pdf/kuznetsov2024roadmap.pdf)