REVIEW 3 major objections 6 minor 42 references
High resolution meta-stereomicroscope based on birefringent meta-optics
T0 review · 3 major / 6 minor · reviewed 2026-08-15 · deepseek-v4-flash
Pith's one-line read One metalens gives a microscope two eyes and 435 nm 3D vision
desk verdict Solid meta-optics engineering with a convincing lateral-resolution story; the depth claims rest on a synthetic-training pipeline that needs much more evidence before the headline 'simultaneous' resolution is taken at face value. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The central object is the birefringent metalens: a flat lens made of rectangular crystalline-silicon nanopillars whose phase response depends on the polarization of the incident light. Each polarization state sees its own aplanatic phase profile, derived from the generalized laws of refraction and imaging, with the optical axis tilted by 6° to match human binocular viewing angle; this encodes two perspectives into one device while maintaining NA 0.6 under water immersion. The second essential component is a polarization imaging sensor with on-chip polarizers, which separates the two polarization channels and suppresses cross-talk. The third is a stereo neural network combining a stereo-matching subnetwork and a U-Net-based mask subnetwork, which converts the parallax images into a depth map and reconstructs the 3D surface.
What would settle it
Image the same pollen grains with an independent depth-measuring technique such as confocal microscopy or white-light interferometry, and compare the network's reconstructed surfaces with those ground-truth maps; if the root-mean-square error exceeds the reported 730 nm on samples outside the training distribution, or if the network fails to reconstruct depth on a different textured specimen, the central claim of simultaneous high lateral and depth resolution is not supported.
Extended reading notes
Core claim
The central claim is that a fully meta-optical architecture can fundamentally eliminate the field-of-view mismatch that has limited previous metalens-assisted stereomicroscopes. The key component is a single birefringent metalens, working under water immersion at 532 nm with numerical aperture 0.6, that encodes two distinct aplanatic phase profiles into two orthogonal polarization states; x-polarized light forms the left view along one tilted optical axis and y-polarized light forms the right view along another, generating parallax from one flat device. With an on-chip polarization sensor separating the two views, the system simultaneously achieves a lateral resolution of 435 nm and a depth resolution of 1,026 nm, and a stereo neural network trained on synthetic parallax images reconstructs 3D surface morphology at about 5 fps. The authors further show the same architecture works in reflection mode on opaque samples and that a relaxed 70 nm minimum feature size is compatible with scalable manufacturing.
Load-bearing premise
The depth-reconstruction claims rest on the assumption that a stereo neural network trained only on Blender-rendered synthetic parallax images, and calibrated with just three pollen samples, transfers accurately to real microscope images well enough to support the reported 730 nm depth precision and 1,026 nm depth resolution on biological samples.
Editorial extensions
If this is right
- A single metalens plus a polarization sensor can replace the dual objective paths of a conventional stereomicroscope, removing optical-axis alignment and shrinking the system to a 40 mm imaging module.
- Eliminating field-of-view mismatch raises the usable field from about 6.2 µm to 43 µm and the depth of field from 3.3 µm to 8.1 µm relative to the prior metalens-assisted design.
- The architecture works in both transmission and reflection modes, so the same module can image biological specimens and opaque industrial parts such as semiconductor chips.
- The stereo neural network reconstructs 3D surface morphology in real time without axial scanning, making single-shot depth imaging possible at roughly 5 fps.
- The relaxed minimum feature size of 70 nm in the reflection-mode lens points toward roll-to-roll nanoimprint fabrication of the same design.
Reading between the lines
- If the synthetic-to-real transfer holds, the same Blender-trained network should work across metalens designs sharing the same parallax geometry without retraining; testing it on a second metalens of different NA would confirm this.
- The measured depth resolution is likely set by the stereo network and pixel sampling rather than by the metalens optics themselves, so a higher-NA or higher-magnification version of the same system should show better depth precision.
- Because stereo vision only recovers visible surfaces, adding sample micro-rotation or multi-angle illumination could extend the method to full 3D shape recovery, as the authors note.
- The polarization-multiplexing approach could be extended to color or to a conventional Bayer sensor by using achromatic multifunctional metalenses, potentially removing the cost and spatial-frequency penalty of the polarization sensor.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper demonstrates a compact meta-stereomicroscope based on a single birefringent metalens that encodes two tilted, polarization-dependent phase profiles, allowing simultaneous left- and right-view imaging on a polarization sensor. The authors report a lateral resolution of 435 nm (USAF Group 10 Element 2) at 532 nm with an NA of 0.6, a 43 μm FOV, and an 8.1 μm DOF, and claim that this improves on the metalens-assisted stereomicroscope of Ref. [15] by removing the FOV mismatch. Depth information is recovered with a stereo neural network trained on 7,000 Blender-rendered parallax image pairs, calibrated on three pollen samples, and validated on eight additional pollen samples, yielding a claimed depth precision of 730 nm RMSE and a depth resolution of 1026 nm. The system is also demonstrated in reflection mode using a larger 2-mm-diameter metalens fabricated with relaxed feature sizes, with correspondingly lower resolution. The central claim is that this is the first fully meta-optical stereo microscope that simultaneously provides 435 nm lateral and 1026 nm depth resolution in a compact, alignment-free module.
Significance. If the depth claims hold, this is a substantial advance in integrated meta-optical microscopy: the single-metalens, polarization-multiplexed architecture is elegant, the lateral-resolution evidence is strong, and the compact 40 mm imaging module with a demonstrated 435 nm half-pitch resolution and a 43 μm FOV is a genuine improvement over prior metalens-assisted stereomicroscopes. The experimental MTF measurements (1236/1233 lp/mm cutoff at 0.1 contrast) are consistent with the design NA of 0.6, and the FOV/DOF comparison against Ref. [15] is a useful quantitative benchmark. The principal weakness is the depth-reconstruction pipeline: the stereo network is trained only on synthetic Blender renders, with no demonstrated matching of the real metalens PSF, aberrations, or noise, and the validation set is restricted to pollen grains of the same class as the calibration set. Because the abstract and conclusions explicitly rest on simultaneous high lateral and depth resolution, the depth-validation protocol is load-bearing and must be strengthened before the headline claim is fully supported.
major comments (3)
- [3D Surface Morphological Reconstruction] The stereo network is trained exclusively on 7,000 Blender-rendered parallax image pairs, and the paper does not provide any quantitative comparison between the rendered image statistics and the real meta-stereomicroscope images, such as MTF/PSF agreement, polarization-dependent aberrations, illumination profiles, or noise levels. The calibration set is only three pollen samples and the validation set is eight additional pollen samples of the same biological class. This leaves open the possibility that the network learns pollen-specific monocular shape or texture priors rather than geometric parallax, so the reported 730 nm RMSE and 1026 nm depth resolution do not yet demonstrate general 3D surface reconstruction for arbitrary real micrographs. Since the abstract and conclusions present the 1026 nm depth resolution as a central result, this domain-gap issue is load-bearing and needs to be addressed with either a non-pollen validation target, a quantitative synthetic-to-real PSF comparison, or an explicit demonstration that the network relies on disparity rather than class-specific cues.
- [3D Surface Morphological Reconstruction] The text states that Blender depth information is calibrated using an electrically driven microscope (Zeiss Axio Observer 7) and that the validation RMSE is computed against ground-truth sample depths, but it does not explain how this microscope provides accurate 3D surface ground truth for pollen grains with complex three-dimensional morphology, nor what the accuracy of that ground truth is. Without a description of the ground-truth acquisition protocol and its uncertainty, the 730 nm RMSE cannot be interpreted as a validated depth-precision metric for the meta-stereomicroscope.
- [3D Surface Morphological Reconstruction] The depth resolution is defined as the minimum distinguishable vertical distance between two planes and is measured by translating a resolution target along z with a motorized stage. This protocol characterizes the system's ability to detect defocus or parallax changes of a flat target, but it does not directly measure the network's ability to reconstruct continuous surface morphology from real biological samples. The 1026 nm value is therefore not by itself sufficient to support the claim of 'simultaneous high lateral and depth resolution imaging' on the pollen images in Fig. 3(g); the connection between the flat-target depth-resolution measurement and the biological surface-reconstruction claim should be justified or the claim should be qualified.
minor comments (6)
- [Design, Fabrication, and Characterization of the Birefringent Metalens] Equations (1) and (2) are corrupted in the manuscript text; the phase-profile formulas need to be typeset correctly so that the aplanatic phase and the sign convention for the two polarization channels are readable.
- [Meta-Stereomicroscope in Transmission Mode] The design phase profile assumes a magnification of 8 and L = tanθ(s+v), while the operating configuration uses s = 0.45 mm and v = 7.8 mm, corresponding to a magnification of 23; the relationship between the design magnification and the operating magnification should be stated explicitly.
- [Meta-Stereomicroscope in Transmission Mode] The sentence 'The maximum resolvable spatial frequency of the sensor is 72 lp/mm' should be reconciled with the later statement that the sensor imposes an object-plane limit of 1665 lp/mm at 23× magnification; please state clearly which figures refer to the sensor plane and which to the object plane.
- [3D Surface Morphological Reconstruction] Fig. 4 and its caption refer to the right panel showing the 3D reconstruction, but the reconstruction is also shown merged with the bright-field image in Fig. 3(g); the relationship between these two displays should be made explicit.
- [Reflection Mode] The reflection-mode section reports 'the maximum resolvable spatial frequency at the sensor plane is 840 lp/mm', which appears inconsistent with the earlier '72 lp/mm' sensor figure; please clarify whether these are sensor-plane versus object-plane quantities or whether different sensors are used.
- [Discussion and Conclusion] The statement that the system achieves 'more than a twofold precision improvement over conventional stereoscopic systems whose depth precision is worse than 1800 nm' relies on Section S10 of the Supplement; the comparison values should be summarized in the main text or in a table so the claim can be assessed without the Supplement.
Circularity Check
No significant circularity: the central optical and depth claims are supported by direct measurements and independent validation, not by fitted inputs or self-referential derivations.
full rationale
The paper's derivation chain is experimentally self-contained. The two phase profiles in Eqs. (1)-(2) are constructed from the stated stereoscopic imaging geometry (object/image distances, observation angle θ=6°, and magnification), and the metalens performance is then assessed by FDTD simulations, measured MTFs, USAF resolution targets, and measured DOF—none of these reported lateral-resolution numbers are fitted parameters used as predictions. The 435 nm lateral resolution is a direct USAF Group 10 Element 2 measurement. The depth claims rest on a stereo neural network trained on Blender-rendered parallax pairs, with the rendering-coordinate depth calibrated to real distances using a Zeiss microscope, followed by a 730 nm RMSE validation on eight unseen pollen samples and a separately measured 1026 nm depth resolution obtained by translating a resolution target with a motorized stage. The only fitted element is the Blender-to-real depth calibration scale, and the headline depth resolution and validation RMSE are not that fitted value; they are independent measurements on unseen data. The self-citations ([15], [19]) are prior experimental/design references used as baseline context and design guidance, not as load-bearing proof of the present claims, and [15] is an externally published, falsifiable result. The synthetic-to-real transfer of the neural network is a legitimate correctness and generalization risk, but it is not a circularity: the network output is compared against real ground-truth depths rather than being defined by them. Therefore no step reduces by construction to its own inputs, and the circularity score is 0.
Assumptions & free parameters
free parameters (1)
- Depth calibration scale (Blender units to real distance) =
Not specified
assumptions (4)
- domain assumption Aplanatic imaging phase profile (Eqs. 1-2) derived from the generalized laws of refraction provides aberration-free tilted-axis imaging for each polarization.
- domain assumption The rectangular c-Si meta-atom library provides independent, full 2π phase control for x and y polarization at 532 nm with acceptable transmittance.
- ad hoc to paper Synthetic Blender-rendered parallax images faithfully represent the optical geometry, aberrations, and texture of the real meta-stereomicroscope for stereo network training.
- standard math Standard stereo geometry: depth varies with disparity through the tilt angle θ and system magnification, and the neural network recovers the same disparity-depth mapping as the physical system.
Cite this review
Pith. "Pith review of High resolution meta-stereomicroscope based on birefringent meta-optics." pith.science (2026). https://pith.science/paper/3ZTZ4MQD
@misc{pith2026260803300,
author = {Pith},
title = {Pith review of: High resolution meta-stereomicroscope based on birefringent meta-optics},
year = {2026},
howpublished = {\url{https://pith.science/paper/3ZTZ4MQD}},
note = {Machine review of arXiv:2608.03300}
}
read the original abstract
Achieving both high lateral and high depth resolution is a longstanding goal in stereomicroscopy. Although meta-optics have revolutionized lens design by alleviating the physical constraints of conventional optical architectures, existing metalens-assisted stereomicroscopes still suffer from field of view (FOV) mismatch between meta-optical and conventional optical components in stereomicroscopes, thereby limiting their imaging performance. Here, we show that this mismatch can be fundamentally eliminated through a fully meta-optical architecture. The integrated system enables flexible control of numerical aperture and magnification with larger depth of field (DOF) and FOV than those of the metalens-assisted stereomicroscopes. Experimentally, we achieve an integrated meta-stereomicroscope with a lateral resolution of 435 nm, surpassing the performance of previously reported stereomicroscopes. Empowered by a stereo neural network, the system enables straightforward reconstruction of high-resolution three-dimensional surface morphology with a depth resolution of 1026 nm, demonstrating the capability to simultaneously achieve high lateral and depth resolution imaging. This integrated architecture operates in both transmission and reflection modes for biomedical imaging and industrial inspection, highlighting its broad applicability for real-time observation across biomedical and industrial scenarios.
Figures
Figures from the paper (2 more)
Reference graph
Works this paper leans on
-
[15]
Metalens-based stereoscopic microscope,
Y. Long, J. Zhang, Z. Liu, W. Feng, S. Guo, Q. Sun, Q. Wu, X. Yu, J. Zhou, E. R. Martins, H. Liang, and J. Li, "Metalens-based stereoscopic microscope," Photon. Res. 10(6), 1501- 1508 (2022) [doi:10.1364/PRJ.456638]
-
[1]
Cell Surface Deformation during an Action Potential,
C. Fillafer, M. Mussel, J. Muchowski, and M. F. Schneider, "Cell Surface Deformation during an Action Potential," Biophys. J. 114(2), 410-418 (2018) [doi:10.1016/j.bpj.2017.11.3776]
-
[2]
TSV reveal height and bump dimension metrology by the TSOM method,
V. Vartanian, R. Attota, H. Park, G. Orji, and R. A. Allen, "TSV reveal height and bump dimension metrology by the TSOM method," in Metrology, Inspection, and Process Control for Microlithography XXVII, Proc. SPIE 8681, 86812F (2013) [doi:10.1117/12.2012609]
-
[3]
Lens-free reflective topography for high-resolution wafer inspection,
H. Lee, J. Sung, S. Park, J. Shin, H. Kim, W. Kim, and M. Lee, "Lens-free reflective topography for high-resolution wafer inspection," Sci. Rep. 14(1), 10519 (2024) [doi:10.1038/s41598-024-59496-4]
-
[4]
Modeling the Depth Resolution of Translucent Layers in Confocal Microscopy,
M. Maier and T. Böhm, "Modeling the Depth Resolution of Translucent Layers in Confocal Microscopy," Small Sci. 4(9), 2400120 (2024) [doi:10.1002/smsc.202400120]
-
[5]
Resolution enhancement of digital holographic microscopy via synthetic aperture: a review,
P. Gao and C. Yuan, "Resolution enhancement of digital holographic microscopy via synthetic aperture: a review," Light Adv. Manuf. 3(1), 105-120 (2022) [doi:10.37188/lam.2022.006]
-
[6]
Quantitative Phase Imaging: Recent Advances and Expanding Potential in Biomedicine,
T. L. Nguyen, S. Pradeep, R. L. Judson-Torres, J. Reed, M. A. Teitell, and T. A. Zangle, "Quantitative Phase Imaging: Recent Advances and Expanding Potential in Biomedicine," ACS Nano. 16(8), 11516-11544 (2022) [doi:10.1021/acsnano.1c11507]
-
[7]
K. Gastinger, K. H. Haugholt, M. Kujawinska, M. Jozwik, C. Schaeffel, and S. Beer, "Optical, mechanical, and electro-optical design of an interferometric test station for massive parallel inspection of MEMS and MOEMS," in Optical Measurement Systems for Industrial Inspection VI, Proc. SPIE 7389, 73891J (2009) [doi:10.1117/12.828162]
Show all 42 references
-
[8]
Spatiotemporal-multiplexed Fourier ptychographic diffraction tomography for high- speed, label-free 3D imaging of live cells,
S. Zhou, Q. Shen, H. Ullah, K. Du, L. Lu, H. Wu, Y. Fan, J. Sun, D. Jin, Q. Chen, and C. Zuo, "Spatiotemporal-multiplexed Fourier ptychographic diffraction tomography for high- speed, label-free 3D imaging of live cells," Adv. Photon. 8(2), 026003 (2026) [doi:10.1117/1.AP.8.2.026003]
2026 doi
-
[9]
Application of Stereomicroscope in the Pre-Analytic Macroscopic Examination of Biopsy Specimens,
M. Jacob, N. Mohan, S. M. Fenn, P. Rajathi, P. Suryagopan, and L. Vishalini, "Application of Stereomicroscope in the Pre-Analytic Macroscopic Examination of Biopsy Specimens," J. Clin. Diagn. Res. 13(10), ZC01-ZC07 (2019) [doi:10.7860/JCDR/2019/42116.13182]
2019
-
[10]
I. P. Howard and B. J. Rogers, Seeing in Depth: Volume 1: Basic Mechanisms/Volume 2: Depth Perception, Oxford University Press, Oxford (2008)
2008
-
[11]
What is binocular disparity?,
J. S. Lappin, "What is binocular disparity?," Frontiers in psychology. 5, 870 (2014) [doi:10.3389/fpsyg.2014.00870]
2014
-
[12]
Four-dimensional imaging based on a binocular chiral metalens,
L. Zhang, J. Yang, L. Zhang, X. Jing, C. Liang, C. Zhang, C. Xiong, Z. Zhang, B. Ma, F. Xing, and X. Zhao, "Four-dimensional imaging based on a binocular chiral metalens," Opt. Lett. 50(3), 1017-1020 (2025) [doi:10.1364/OL.545263]
2025 doi
-
[13]
Miniaturized high-efficiency snapshot polarimetric stereoscopic imaging,
B. Fu, X. Zhou, T. Li, H. Zhu, Z. Liu, S. Zheng, Y. Zhou, Y. Yu, X. Cao, S. Wang, Z. Wang, and S. Zhu, "Miniaturized high-efficiency snapshot polarimetric stereoscopic imaging," Optica. 12(3), 391-398 (2025) [doi:10.1364/OPTICA.549864]
2025 doi
-
[14]
Non-Interleaved Shared-Aperture Full-Stokes Metalens via Prior-Knowledge-Driven Inverse Design,
Y. Wang, Y. Wang, A. Yu, M. Hu, Q. Wang, C. Pang, H. Xiong, Y. Cheng, and J. Qi, "Non-Interleaved Shared-Aperture Full-Stokes Metalens via Prior-Knowledge-Driven Inverse Design," Adv. Mater. 37(8), e2408978 (2025) [doi:10.1002/adma.202408978]
2025 doi
-
[16]
Compact inverted digital holographic microscope based on common-path configuration,
I. Javed, M. B. Hassan, R. Khalid, M. Dashtdar, L. G. Garcia, C. Fonda, M. L. Crespo, M. Danailov, D. Cojoc, M. Zubair, M. Q. Mehmood, and H. Cabrera, "Compact inverted digital holographic microscope based on common-path configuration," Appl. Opt. 64(7), B65-B71 (2025) [doi:10...
2025 doi
-
[17]
Compact stereo endoscopic camera using microprism arrays,
S. P. Yang, J. J. Kim, K. W. Jang, W. K. Song, and K. H. Jeong, "Compact stereo endoscopic camera using microprism arrays," Opt. Lett. 41(6), 1285-1288 (2016) [doi:10.1364/OL.41.001285]
2016 doi
-
[18]
Imaging performance of a miniature integrated microendoscope,
J. D. Rogers, S. Landau, T. S. Tkaczyk, M. R. Descour, M. S. Rahman, R. Richards- Kortum, A. H. O. Kärkäinen, and T. Christenson, "Imaging performance of a miniature integrated microendoscope," J. Biomed. Opt . 13(5), 054020 (2008) [doi:10.1117/1.2978060]
2008 doi
-
[19]
High performance metalenses: numerical aperture, aberrations, chromaticity, and trade- offs,
H. Liang, A. Martins, B. H. V. Borges, J. Zhou, E. R. Martins, J. Li, and T. F. Krauss, "High performance metalenses: numerical aperture, aberrations, chromaticity, and trade- offs," Optica. 6(12), 1461-1470 (2019) [doi:10.1364/OPTICA.6.001461]
2019 doi
-
[20]
High-efficiency broadband achromatic metalens for near-IR biological imaging window,
Y. Wang, Q. Chen, W. Yang, Z. Ji, L. Jin, X. Ma, Q. Song, A. Boltasseva, J. Han, V. M. Shalaev, and S. Xiao, "High-efficiency broadband achromatic metalens for near-IR biological imaging window," Nat. Commun. 12(1), 5560 (2021) [doi:10.1038/s41467-021- 25797-9]
2021 doi
-
[21]
Meta-grating-lens-based monolithic polarization camera,
F. J. Li, Z. Feng, Z. Wan, T. Shi, S. Qiu, J. H. Zeng, S. Song, S. Wang, Z. L. Deng, and X. Li, "Meta-grating-lens-based monolithic polarization camera," Sci. Adv. 11(43), eadx9886 (2025) [doi:10.1126/sciadv.adx9886]
2025 doi
-
[22]
Holographic Super-Resolution Metalens for Achromatic Sub-Wavelength Focusing,
X. Dai, F. Dong, K. Zhang, D. Liao, S. Li, Z. Shang, Y. Zhou, G. Liang, Z. Zhang, Z. Wen, G. Chen, L. Dai, and W. Chu, "Holographic Super-Resolution Metalens for Achromatic Sub-Wavelength Focusing," ACS Photonics. 8(8), 2294-2303 (2021) [doi:10.1021/acsphotonics.1c00411]
2021 doi
-
[23]
Neural nano-optics for high-quality thin lens imaging,
E. Tseng, S. Colburn, J. Whitehead, L. Huang, S. H. Baek, A. Majumdar, and F. Heide, "Neural nano-optics for high-quality thin lens imaging," Nat. Commun. 12(1), 6493 (2021) [doi:10.1038/s41467-021-26443-0]
2021 doi
-
[24]
Chip-scale metalens microscope for wide-field and depth-of-field imaging,
X. Ye, X. Qian, Y. Chen, R. Yuan, X. Xiao, C. Chen, W. Hu, C. Huang, S. Zhu, and T. Li, "Chip-scale metalens microscope for wide-field and depth-of-field imaging," Adv. Photon. 4(4), 046006 (2022) [doi:10.1117/1.AP.4.4.046006]
2022 doi
-
[25]
Plan meta-objective for sub-micron quantitative phase imaging,
J. Wang, J. Sun, J. Li, C. Huang, J. Ji, W. Shen, Z. Wang, J. Zhou, C. Chen, S. Zhu, and T. Li, "Plan meta-objective for sub-micron quantitative phase imaging," Light Sci. Appl. 15(1), 71 (2026) [doi:10.1038/s41377-025-02099-z]
2026 doi
-
[26]
Neural phase microscopy with metasurface optics for real-time and nanoscale quantitative phase imaging,
G. Y. Lee, C. Kim, M. Gopakumar, Y. Kim, B. Lee, Y. Jeong, and G. Wetzstein, "Neural phase microscopy with metasurface optics for real-time and nanoscale quantitative phase imaging," Nat. Commun. 17(1), 1411 (2026) [doi:10.1038/s41467-025-68151-z]
2026 doi
-
[27]
Compound metalens-based miniature two-photon microscope for large-FOV imaging in freely behaving animals,
Z. Hao, Y. Zhang, Y. Zhu, B. Sun, H. Jiao, Y. Hu, Z. Lin, L. Feng, A. Wang, S. Xiao, and R. Wu, "Compound metalens-based miniature two-photon microscope for large-FOV imaging in freely behaving animals," PhotoniX. 6(1), 57 (2025) [doi:10.1186/s43074-025- 00218-y]
2025 doi
-
[28]
Miniature Two-Photon Microscopic Imaging Using Dielectric Metalens,
C. Wang, Q. Chen, H. Liu, R. Wu, X. Jiang, Q. Fu, Z. Zhao, Y. Zhao, Y. Gao, B. Yu, H. Jiao, A. Wang, S. Xiao, and L. Feng, "Miniature Two-Photon Microscopic Imaging Using Dielectric Metalens," Nano Lett . 23(17), 8256-8263 (2023) [doi:10.1021/acs.nanolett.3c02439]
2023 doi
-
[29]
Single-Shot 3D Imaging Meta- Microscope,
H. Hao, H. Wang, X. Wang, X. Ding, S. Zhang, C. F. Pan, M. A. Rahman, T. Ling, H. Li, J. Tan, J. K. W. Yang, W. Lu, J. Liu, and G. Hu, "Single-Shot 3D Imaging Meta- Microscope," Nano Lett. 24(42), 13364-13373 (2024) [doi:10.1021/acs.nanolett.4c03952]
2024 doi
-
[30]
A Light-Field Metasurface for High-Resolution Single-Particle Tracking,
A. L. Holsteen, D. Lin, I. Kauvar, G. Wetzstein, and M. L. Brongersma, "A Light-Field Metasurface for High-Resolution Single-Particle Tracking," Nano Lett. 19(4), 2267-2271 (2019) [doi:10.1021/acs.nanolett.8b04673]
2019 doi
-
[31]
Spectral tomographic imaging with aplanatic metalens,
C. Chen, W. Song, J. W. Chen, J. H. Wang, Y. H. Chen, B. Xu, M. K. Chen, H. Li, B. Fang, J. Chen, H. Y. Kuo, S. Wang, D. P. Tsai, S. Zhu, and T. Li, "Spectral tomographic imaging with aplanatic metalens," Light Sci. Appl. 8(1), 99 (2019) [doi:10.1038/s41377- 019-0208-0]
2019 doi
-
[32]
Single-shot deterministic complex amplitude imaging with a single-layer metalens,
L. Li, S. Wang, F. Zhao, Y. Zhang, S. Wen, H. Chai, Y. Gao, W. Wang, L. Cao, and Y. Yang, "Single-shot deterministic complex amplitude imaging with a single-layer metalens," Sci. Adv. 10(1), eadl0501 (2024) [doi:10.1126/sciadv.adl0501]
2024 doi
-
[33]
Dielectric metasurfaces for complete control of phase and polarization with subwavelength spatial resolution and high transmission,
A. Arbabi, Y. Horie, M. Bagheri, and A. Faraon, "Dielectric metasurfaces for complete control of phase and polarization with subwavelength spatial resolution and high transmission," Nat. Nanotechnol. 10(11), 937-943 (2015) [doi:10.1038/nnano.2015.186]
2015 doi
-
[34]
A golay metalens for long-range, large aperture, thermal imaging via sparse aperture computational imaging,
J. Wang, A. Wirth-Singh, V. Saragadam, R. Johnson, A. Majumdar, and A. Veeraraghavan, "A golay metalens for long-range, large aperture, thermal imaging via sparse aperture computational imaging," Nat. Commun. 16(1), 10281 (2025) [doi:10.1038/s41467-025- 65188-y]
2025 doi
-
[35]
High-resolution and wide-field microscopic imaging with a monolithic meta-doublet under annular illumination,
J. Sun, W. Shen, J. Wang, R. Yu, J. Li, C. Huang, X. Ye, Z. Cheng, J. Yu, P. Wang, C. Chen, S. Zhu, and T. Li, "High-resolution and wide-field microscopic imaging with a monolithic meta-doublet under annular illumination," Adv. Photon. 7(4), 046006 (2025) [doi:10.1117/1.AP.7.4.046006]
2025 doi
-
[36]
High-Frequency Stereo Matching Network,
H. Zhao, H. Zhou, Y. Zhang, J. Chen, Y. Yang, and Y. Zhao, “High-Frequency Stereo Matching Network,” in Proc. IEEE/CVF Conf. Comput. Vis. Pattern Recognit. (CVPR), pp. 1327-1336 (2023) [doi:10.1109/CVPR52729.2023.00134]
2023
-
[37]
XYDeblur: Divide and Conquer for Single Image Deblurring,
S. W. Ji, J. Lee, S. W. Kim, J. P. Hong, S. J. Baek, S. W. Jung, and S. J. Ko, "XYDeblur: Divide and Conquer for Single Image Deblurring," in Proc. IEEE/CVF Conf. Comput. Vis. Pattern Recognit. (CVPR), 17400-17409 (2022) [doi:10.1109/CVPR52688.2022.01690]
2022
-
[38]
300-unit-per-second roll-to-roll manufacturing of visible metalenses,
T. Hoang, Y. Park, J. Kim, H. Truong, S. Parajuli, B. J. Rajasekaran, K. Kim, D. Kang, G. Jeon, K. I. Lee, D. H. Yoon, I. Kim, J. Rho, and G. Cho, "300-unit-per-second roll-to-roll manufacturing of visible metalenses," Nature. 652(8112), 1188-1194 (2026) [doi:10.1038/s41586-02...
2026 doi
-
[39]
Helical opto-thermoviscous flows drive out-of-plane rotation and particle spinning in a highly viscous micro-environment,
F. Nan, W. Liao, A. Puerta, J. Spiegelberg, E. Erben, R. Mikut, S. Allgeier, M. Wegener, E. Lauga, and M. Kreysing, "Helical opto-thermoviscous flows drive out-of-plane rotation and particle spinning in a highly viscous micro-environment," Light Sci. Appl. 15(1), 231 (2026) [d...
2026 doi
-
[40]
Efficient Silicon Metasurfaces for Visible Light,
Z. Zhou, J. Li, R. Su, B. Yao, H. Fang, K. Li, L. Zhou, J. Liu, D. Stellinga, C. P. Reardon, T. F. Krauss, and X. Wang, "Efficient Silicon Metasurfaces for Visible Light," ACS Photonics. 4(3), 544-551 (2017) [doi:10.1021/acsphotonics.6b00740]
2017 doi
-
[41]
Large-area pixelated metasurface beam deflector on a 12-inch glass wafer for random point generation,
N. Li, Y. H. Fu, Y. Dong, T. Hu, Z. Xu, Q. Zhong, D. Li, K. H. Lai, S. Zhu, Q. Lin, Y. Gu, and N. Singh, "Large-area pixelated metasurface beam deflector on a 12-inch glass wafer for random point generation," Nanophotonics. 8(10), 1855-1861 (2019) [doi:10.1515/nanoph-2019-0208]
2019 doi
-
[42]
Silica-embedded silicon photonic crystal waveguides,
T. P. White, L. O'Faolain, J. Li, L. C. Andreani, and T. F. Krauss, "Silica-embedded silicon photonic crystal waveguides," Opt. Express. 16(21), 17076-17081 (2008) [doi:10.1364/OE.16.017076]
2008 doi
Reviewed August 15, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.