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Cavity-assisted nonlocal metasurfaces for momentum-space broadband-operational optical vortice generation with maximum efficiency approaching 80%

Co-first author

Research overview

Problem

Momentum-space singularities enable vortex generation in nonlocal metasurfaces, but steep high-Q dispersion limits bandwidth and conversion efficiency.

Mechanism

A Fabry-Pérot cavity controls coupling between bound states in the continuum (BICs) and degeneracy points, tuning dispersion, radiative Q and polarization into quasi-flat bands with strong scattering.

Result

In Figure 5, efficiency peaks at 77% for NA = 0.24 at 1520 nm. Under the separate conditions of NA = 0.21 at 1520 nm, the l = −2 orbital-angular-momentum purity reaches 91.7%.

Journal
Opto-Electronic Advances
Year
2026
DOI
Read the original paper ↗
Cavity-assisted nonlocal metasurfaces for momentum-space broadband-operational optical vortice generation with maximum efficiency approaching 80%, first article page
First article page · Select to enlarge

Preview versionPublished article · OEA 9, 250296 (2026). The preview starts at the article's first page, after the publisher's cover and front matter.

Turning momentum-space singularities into a vortex converter

Generating phase winding is only part of the problem: light must also convert efficiently over a finite bandwidth and angular range. One mechanism figure and one experimental figure connect the design choices to observations and measurement conditions.

Designing dispersion and radiation together

Figure 2 combines a silicon photonic-crystal slab, a silica spacer and a gold mirror. The spacer forms a tunable Fabry-Pérot cavity; periodic perturbation preserving C4 symmetry introduces Brillouin-zone folding and guided resonances. Coupling BIC- and degeneracy-point-related modes changes dispersion, radiative linewidth and polarization together, producing the two broadband high-efficiency regimes in Figure 2(d). Figures 2(e) and 2(f) compare simulated bands of conventional and optimized designs.

Original Figure 2: the reflective photonic-crystal slab, coupling of BIC- and degeneracy-point-related modes, and bands for conventional and optimized designs.
Figure 2 | Mechanism and numerical design. The spacer forms a Fabry-Pérot cavity and periodic perturbation introduces guided resonances. Mode coupling jointly shapes dispersion, radiative linewidth and polarization. Panels (e) and (f) compare simulated bands of conventional and optimized designs. The original figure number and complete caption are retained.Source: Wang et al., Opto-Electronic Advances 9, 250296 (2026), Fig. 2 ↗ · CC BY 4.0The complete figure and caption were extracted from PDF page 6. Only surrounding text and whitespace were cropped; colors, panels, labels and proportions are unchanged.

Reading the experimental numbers with their illumination conditions

Figure 5(a) compares illumination positions from near the edge to the center; Figure 5(b) measures overall averaged efficiency across wavelength and NA. The text reports a 77% peak at 1520 nm for NA = 0.24, with efficiency above 60% over ±25 nm around that wavelength. Figures 5(c) and 5(d) show beams, phase and LG-mode decomposition at NA = 0.21; the l = −2 purity reaches 91.7% at 1520 nm. These observations examine position dependence, operating range and vortex-mode composition separately.

Original Figure 5: vortex beams at different illumination positions, conversion efficiency versus wavelength and numerical aperture, and intensity, phase and modal decomposition at 1510, 1520 and 1530 nm.
Figure 5 | Experimental results and measurement conditions. Efficiency peaks at 77% at 1520 nm for NA = 0.24. The l = −2 OAM purity is 91.7% at 1520 nm for NA = 0.21. Efficiency and purity were measured at different NAs and do not describe a single operating point. The original figure number and complete caption are retained.Source: Wang et al., Opto-Electronic Advances 9, 250296 (2026), Fig. 5 ↗ · CC BY 4.0The complete figure and caption were extracted from PDF page 10. Only surrounding text and whitespace were cropped; colors, panels, labels and proportions are unchanged.

From a mechanism figure to measured evidence

Together, these figures connect topological singularities and tunable mode coupling to device behavior under finite illumination conditions. Figure 2 contains structural schematics and numerical bands; Figure 5 contains experimental measurements. The 77% efficiency and 91.7% purity have distinct NA and wavelength conditions, rather than being universal specifications. This site's software tracking example uses independent synthetic data and is not presented as a computation used in this paper.

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