- Aug. 17, 2026
- Vol. 14, Issue 7 (2026)
- Aug. 17, 2026
- Vol. 14, Issue 7 (2026)
- Aug. 17, 2026
- Vol. 14, Issue 7 (2026)
- Aug. 14, 2026
- Vol. , Issue (2026)
- Aug. 14, 2026
- Vol. , Issue (2026)
Tailoring the properties of the driving laser to the need of applications often requires compromises among laser stability, high peak and average power lev
Tailoring the properties of the driving laser to the need of applications often requires compromises among laser stability, high peak and average power levels, pulse duration, and spectral bandwidth. For instance, spectroscopy with optical frequency combs in the extreme/visible ultraviolet spectral region requires a high peak power of the near-IR driving laser, and therefore high average power, pulse duration of a few tens of fs, and maximal available spectral bandwidth. Contrarily, the parametric conversion efficiency is higher for pulses with a duration in the 100-fs range due to temporal walk-off and coating limitations. Here we suggest an approach to adjust the spectral characteristics of high-power chirped-pulse amplification (CPA) to the requirements of different nonlinear frequency converters while preserving the low-phase-noise (PN) properties of the system. To achieve spectral tunability, we installed a mechanical spectral shaper in a free-space section of the stretcher of an in-house-developed ytterbium-fiber-based CPA system. The CPA system delivers 100 W of average power at a repetition rate of 132.4 MHz. While gaining control over the spectral properties, we preserve the relative-intensity-noise and PN properties of the system. The high-power CPA can easily be adjusted to deliver either a spectrum ideal for mid-IR light generation (full width at half maximum of ∼11 nm, compressed pulse duration of 230 fs) or a spectrum ideal for highly nonlinear processes such as high-harmonic generation (-10 dB level of >50 nm, transform-limited pulse duration of ∼65 fs).show less
- Aug.17,2026
- Photonics Research,Vol. 10, Issue 10
- 2309 (2022)
By reconstructing 2D images of an object using temporal signals captured by a single-pixel photodetector (PD), single-pixel imaging (SPI) technology offers
By reconstructing 2D images of an object using temporal signals captured by a single-pixel photodetector (PD), single-pixel imaging (SPI) technology offers a cost-effective alternative to traditional focal-plane-array imaging systems. This advantage is particularly significant in some non-visible spectral bands, where manufacturing PD arrays is prohibitively expensive. However, conventional SPI systems, which employ single-beam structured light, suffer from limited imaging speeds. In this paper, we propose a multi-beam structured light SPI (MSL-SPI) system. It combines the spatial modulation scheme and the parallel measurement capabilities of a dual-comb interferometer. Compared with traditional SPI systems, the imaging speed can be significantly improved without compromising the space-bandwidth product. Experiments were performed to verify the system, which achieved simultaneous spatial modulation on nine light beams, improving the imaging speed by approximately an order of magnitude. Sub-second temporal resolution and a pixel count of 12×12 were realized using a standard digital micromirror device (DMD) with a refresh rate of only 60 Hz. Furthermore, dynamic imaging with a frame rate of 30 frames per second (FPS) and a pixel count of 6×6 was demonstrated under a 240 Hz refresh rate of the DMD. These results showcase the potential of MSL-SPI for faster and more efficient SPI systems.show less
- Aug.13,2026
- Advanced Imaging,Vol. 3, Issue 5
- 051001 (2026)
Leveraging the natural axial confinement of coherent extreme ultraviolet (EUV) light generated via the high-order harmonic generation process, we demonstra
Leveraging the natural axial confinement of coherent extreme ultraviolet (EUV) light generated via the high-order harmonic generation process, we demonstrate the spatial separation of EUV and the driving infrared (IR) beams through hollow-core microchannels embedded in a laser machine glass device. This structure enables broadband EUV transmission while attenuating the collinear IR by 2 orders of magnitude. In addition, we explore the potential of integrated photonic architectures based on EUV-guiding hollow structures, laying the foundation for a new class of compact, palm-top devices for EUV and soft X-ray applications.show less
- Aug.12,2026
- Advanced Photonics Nexus,Vol. 5, Issue 4
- 046025 (2026)
Applications of terawatt-class lasers can enormously benefit from pulse trains with kHz repetition rates. The associated unprecedented combinations of peak
Applications of terawatt-class lasers can enormously benefit from pulse trains with kHz repetition rates. The associated unprecedented combinations of peak and average powers require the development of new concepts for scalable ultrashort pulse generation. Through comprehensive simulations, we analyze spectral broadening of 300-ps, 100-mJ pulses in multi-pass cells and anti-resonant hollow-core fibers towards the fs regime. We introduce an 11-mirror cell geometry that can deliver kilometer-scale nonlinear interaction lengths. We experimentally demonstrate nearly 300 passes in such a cell. This enables at least four times larger B-integral to peak power ratios than in previously reported spectral broadening experiments with air-filled multi-pass cells. These results highlight the strong potential of advanced multi-pass cell designs to reach unprecedented broadening factors. The proposed scheme can efficiently transform industrially mature high-power, high-energy lasers into unique ultrafast sources.show less
- Aug.11,2026
- High Power Laser Science and Engineering,Vol. 14, Issue 4
- 04000e69 (2026)
Photonic neuromorphic computing promises revolutionary advances in parallel and high-speed processing, yet a key challenge persists: co-integrating nonlinearity, dense connectivity, and intrinsi
Photonic neuromorphic computing promises revolutionary advances in parallel and high-speed processing, yet a key challenge persists: co-integrating nonlinearity, dense connectivity, and intrinsic memory monolithically to enable brain-inspired, spatiotemporal information processing. Here, we overcome this challenge by introducing a monolithic photonic neural network based on a metasurface operating at bound state in the continuum (BIC). The BIC mode mediates strong, long-range coupling across the lattice, supporting a reconfigurable recurrent network topology in hardware. Concurrently, the gain medium provides both optical nonlinearity for neuronal activation and a finite carrier lifetime that serves as a built-in, analog temporal memory. This synergy enables computation to emerge directly from the collective spatiotemporal dynamics of the driven-dissipative photonic system, effectively realizing a physical reservoir computer on a chip. We experimentally validate a minimal yet physically complete system on benchmark tasks—brain MRI image classification and human action recognition—achieving 92.16% and 85.25% accuracies, respectively. This work establishes a scalable pathway toward ultrafast, energy-efficient neuromorphic intelligence where processing is an inherent property of tailored light–matter interaction.show less
- Aug.14,2026
- Advanced Photonics,Vol. 8, Issue 5
- (2026)
Fiber-optic imaging enables flexible, minimally invasive, deep-tissue imaging of otherwise inaccessible biological targets using optical fiber devices. Methods based on direct signal measurement
Fiber-optic imaging enables flexible, minimally invasive, deep-tissue imaging of otherwise inaccessible biological targets using optical fiber devices. Methods based on direct signal measurements have been widely adopted in biomedical research and clinical applications. However, imaging performance is bottlenecked by limited modal capacity, fiber-induced distortion, and reduced robustness. Driven by advances in fiber optics and modern computational imaging, computational fiber-optic imaging methods can effectively address these challenges, enabling high-fidelity, robust fiber-optic imaging that benefits fundamental research and clinical practice. This review first introduces the significance and challenges of direct fiber-optic imaging methods and contrasts their framework with that of computational fiber-optic imaging. Major optical-fiber devices and representative computational fiber-optic imaging strategies are then reviewed. Finally, the imaging performance and applications of established computational approaches, as well as future directions, are discussed and synthesized.show less
- Aug.13,2026
- Advanced Photonics Nexus,Vol. 5, Issue 6
- (2026)
Single-photon imaging is an advanced optical technology that uses single-photon detectors to capture extremely weak light signals or individual photons carrying quantum information. It achieves
Single-photon imaging is an advanced optical technology that uses single-photon detectors to capture extremely weak light signals or individual photons carrying quantum information. It achieves high sensitivity, high temporal resolution, and multi-dimensional imaging by relying on single-photon detectors. Among many single-photon detection technologies, superconducting nanowire single-photon detectors (SNSPDs) have demonstrated superior performance and are widely used in both quantum information science and classical light-detection scenarios. Expanding single-pixel SNSPD detectors into large-scale arrays and integrating them with cryogenic systems, imaging optics, reconstruction algorithms, and other auxiliary units to build a practical high-performance single-photon camera is an inspiring goal in the community and will surely promote single-photon imaging applications. Although this task is difficult and challenging for superconducting electronics, significant progress has already been made. This review summarizes the developmental history of SNSPD arrays, various readout architectures, and remaining challenges, aiming to encourage cross-disciplinary research to accelerate the deployment and implementation of SNSPD cameras.show less
- Aug.13,2026
- Advanced Imaging,Vol. 3, Issue 4
- (2026)
With the advent of the Quantum 2.0 era, technologies increasingly exploit nonclassical properties of quantum mechanics. Quantum imaging (QI) uses nonclassical phenomena such as quantum entanglem
With the advent of the Quantum 2.0 era, technologies increasingly exploit nonclassical properties of quantum mechanics. Quantum imaging (QI) uses nonclassical phenomena such as quantum entanglement, antibunching, and squeezing to develop new imaging modalities and enhance existing biomedical imaging techniques. Although QI has the potential to surpass certain classical limitations in biomedical imaging, it has seen limited adoption in biomedicine. This limited adoption may reflect a knowledge gap between the QI and biomedical imaging communities. In this review, we introduce biomedical QI through an overview and comparison of the key QI properties and methods relevant to biomedical imaging. We discuss fundamentally new methods enabled by QI, such as quantum ghost imaging, quantum imaging with undetected photons, and biphoton imaging, while also reviewing biomedical imaging methods that QI has already enhanced. Additionally, we compare the performance characteristics of quantum imaging cameras and representative biomedical QI methods. Finally, we discuss the limitations of QI and the factors that may limit future biomedical QI research.show less
- Aug.13,2026
- Advanced Imaging,Vol. 3, Issue 4
- (2026)
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- Aug. 17, 2026
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- Aug. 17, 2026
















