Diffractive beam splitter into a 7 × 7 spot array
Design an etched silica splitter that divides a 632.8 nm beam into a 7 × 7 array of equal beams, maximizing efficiency times uniformity.
| 1 | # Diffractive beam splitter into a 7 × 7 spot array |
| 2 | |
| 3 | Design an etched glass surface that splits one laser beam into 49 beams of equal power, fanning out over ±15°. Such splitters are used in structured-light projection and multifocal microscopy, and the hard part is to keep both the total efficiency high and the 49 beams equal at the same time. |
| 4 | |
| 5 | ## Task |
| 6 | |
| 7 | The device is a biperiodic pattern etched in silica (SiO₂, refractive index 1.46) with a 7.2 µm × 7.2 µm unit cell. A design consists of a binary etch pattern on a 40 nm grid (180 × 180 pixels), the thickness of the patterned layer in $[0.5,1.5]$ µm, and the thicknesses of two thin auxiliary layers, each in $[0,0.1]$ µm. A TE-polarized 632.8 nm plane wave arrives from air at normal incidence. Let $\eta_{(i,j)}$ be the efficiency of the transmitted diffraction order $(i,j)$, for $i,j\in\{-3,\dots,3\}$, summed over the two output polarizations (TE→TE plus TE→TM). With total efficiency $T=\sum_{i,j}\eta_{(i,j)}$ and uniformity error |
| 8 | |
| 9 | $$U=\frac{\max_{i,j}\eta_{(i,j)}-\min_{i,j}\eta_{(i,j)}}{\max_{i,j}\eta_{(i,j)}+\min_{i,j}\eta_{(i,j)}},$$ |
| 10 | |
| 11 | the score is |
| 12 | |
| 13 | $$\mathcal{M}=T\,(1-U),$$ |
| 14 | |
| 15 | higher is better (a perfect splitter scores 1). A valid design is fully binary, with minimum feature width and minimum gap of at least 10 pixels (400 nm), measured with the imageruler package, the challenge's default target. |
| 16 | |
| 17 | ## Background |
| 18 | |
| 19 | The problem follows a LightTrans case study of a non-paraxial diffractive beam splitter, whose designs used a grid of square pillars and a hybrid of the iterative Fourier transform algorithm, the thin-element approximation and a final rigorous coupled-wave analysis. Schubert (2024) implemented it in the invrs-gym with the FMMAX Fourier modal method, which matches the LightTrans results closely and is fast enough to optimize with the accurate model throughout. The published designs suggest a trade-off between total efficiency and uniformity, so the problem is a natural test for multi-objective optimization and for how the two goals are combined into one score. |
| 20 | |
| 21 | ## Data and evaluation |
| 22 | |
| 23 | - **Instance:** one fixed device, `invrs_gym.challenges.diffractive_splitter()` with default arguments. |
| 24 | - **Evaluation code:** the [invrs leaderboard](https://github.com/invrs-io/leaderboard) scorer (`invrs_leaderboard.utils.evaluate_solutions_to_challenge`), on CPU in 64-bit precision with about 1000 Fourier terms. It also reports the minimum width and spacing in pixels. Submissions are `totypes` JSON parameter files. |
| 25 | - **Hardware:** none assumed; the score does not depend on run time. |
| 26 | |
| 27 | ## What is known |
| 28 | |
| 29 | - The LightTrans designs, re-simulated by Schubert (2024), have total efficiencies of about 0.68 to 0.74 but uniformity errors between 0.40 and 0.80, so their scores stay below 0.45. |
| 30 | - Best on the final leaderboard: 0.5964, a design by M. F. Schubert (April 2024) with 400 nm features, total efficiency 0.641 and uniformity error 0.069. |
| 31 | - All 24 leaderboard designs meet the 400 nm target and all come from the gym's author. |
| 32 | |
| 33 | ## What would count as progress |
| 34 | |
| 35 | - A binary design meeting the 400 nm target with $\mathcal{M}>0.5964$, re-scored with the leaderboard code. |
| 36 | - A design with total efficiency above 0.70 and uniformity error below 0.10, which no leaderboard design reaches. |
| 37 | - A justified upper bound on $T$ for a single binary etched layer, to show how much room is left. |
| 38 | |
| 39 | ## References |
| 40 | |
| 41 | 1. M. F. Schubert. invrs-gym: a toolkit for nanophotonic inverse design research. 2024. [arXiv:2410.24132](https://arxiv.org/abs/2410.24132) |
| 42 | 2. LightTrans. Design and rigorous analysis of non-paraxial diffractive beam splitter (use case, version 3.1). [LightTrans](https://www.lighttrans.com/use-cases/application/design-and-rigorous-analysis-of-non-paraxial-diffractive-beam-splitter.html) |
| 43 | 3. M. F. Schubert, A. M. Hammond. Fourier modal method for inverse design of metasurface-enhanced micro-LEDs. Optics Express 31, 42945 (2023). [doi:10.1364/OE.503481](https://doi.org/10.1364/OE.503481) |
| 44 | 4. invrs.io. Diffractive splitter leaderboard (final state, archived October 2025). [Leaderboard page](https://invrs-io.github.io/leaderboard/notebooks/leaderboards/diffractive_splitter.html) |
| 45 | |
| 46 | ## Source |
| 47 | |
| 48 | Imported from [invrs-gym diffractive_splitter](https://invrs-io.github.io/gym/notebooks/challenges/diffractive_splitter.html), curated by Martin F. Schubert (invrs.io). The gym and its leaderboard were archived in October 2025 and no longer take submissions; the scores above are the leaderboard's final state. The statement above is written in our own words; see the source for the original wording, history and discussion. |