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A silicon photonics waveguide-coupled colloidal quantum dot photodiode sensitive beyond 1.6 µm 灵敏度超过 1.6 µm 的硅光子波导耦合胶体量子点光电二极管
IF 5.6 1区 物理与天体物理 Q1 OPTICS Pub Date : 2024-06-20 DOI: 10.1063/5.0206386
Chao Pang, Yu-hao Deng, Ezat Kheradmand, Luis Moreno Hagelsieb, Yujie Guo, David Cheyns, Pieter Geiregat, Zeger Hens, Dries Van Thourhout
Silicon photonics faces a persistent challenge in extending photodetection capabilities beyond the 1.6 µm wavelength range, primarily due to the lack of appropriate epitaxial materials. Colloidal quantum dots present a promising solution here, offering distinct advantages, such as infrared wavelength tunability, cost-effectiveness, and facile deposition. Their unique properties position them as a potential candidate for enabling photodetection in silicon photonics beyond the conventional telecom wavelength, thereby expanding the potential applications and capabilities within this domain. In this study, we have successfully integrated lead sulfide (PbS) colloidal quantum dot photodiodes (QDPDs) onto silicon waveguides using standard process techniques. The integrated photodiodes exhibit a remarkable responsivity of 1.3 A/W (with an external quantum efficiency of 74.8%) at a wavelength of 2.1 µm, a low dark current of only 106 nA, and a bandwidth of 1.1 MHz under a −3 V bias. To demonstrate the scalability of our integration approach, we have developed a compact 8-channel spectrometer incorporating an array of QDPDs. This achievement marks a significant step toward realizing a cost-effective photodetector solution for silicon photonics, particularly tailored for a wide range of sensing applications around the 2 µm wavelength range.
硅光子学在将光电探测能力扩展到 1.6 µm 波长范围之外方面一直面临挑战,这主要是由于缺乏合适的外延材料。胶体量子点是一种很有前景的解决方案,具有红外波长可调、成本效益高和易于沉积等显著优势。胶体量子点的独特性能使其成为硅光子学中实现传统电信波长以外光电探测的潜在候选材料,从而拓展了这一领域的潜在应用和能力。在这项研究中,我们利用标准工艺技术成功地将硫化铅(PbS)胶体量子点光电二极管(QDPD)集成到了硅波导上。集成的光电二极管在 2.1 µm 波长下的响应率高达 1.3 A/W(外部量子效率为 74.8%),暗电流低至 106 nA,在 -3 V 偏置下的带宽为 1.1 MHz。为了证明我们的集成方法的可扩展性,我们开发了一种集成了 QDPD 阵列的紧凑型 8 通道光谱仪。这一成果标志着我们在为硅光子学实现经济高效的光电探测器解决方案方面迈出了重要一步,尤其是为 2 µm 波长范围内的各种传感应用量身定制的光电探测器解决方案。
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引用次数: 0
Unsupervised learning enables multicolor synchronous fluorescence microscopy without cytoarchitecture crosstalk 无监督学习可实现多色同步荧光显微镜观察,且无细胞结构串扰
IF 5.6 1区 物理与天体物理 Q1 OPTICS Pub Date : 2024-05-30 DOI: 10.1063/5.0202622
Bolin Lu, Zhangheng Ding, Kefu Ning, Xiaoyu Zhang, Xiangning Li, Jiangjiang Zhao, Ruiheng Xie, Dan Shen, Jiahong Hu, Tao Jiang, Jianwei Chen, Hui Gong, Jing Yuan
In multicolor fluorescence microscopy, it is crucial to orient biological structures at a single-cell resolution based on precise anatomical annotations of cytoarchitecture images. However, during synchronous multicolor imaging, due to spectral mixing, the crosstalk from the blue signals of 4′,6-diamidino-2-phenylindole (DAPI)-stained cytoarchitecture images to the green waveband hinders the visualization and identification of green signals. Here, we proposed a deep learning-based framework named the crosstalk elimination and cytoarchitecture enhancement pipeline (CECEP) to simultaneously acquire crosstalk-free signals in the green channel and high-contrast DAPI-stained cytoarchitecture images during multicolor fluorescence imaging. For the CECEP network, we proposed an unsupervised learning algorithm named the cytoarchitecture enhancement network (CENet), which increased the signal-to-background ratio (SBR) of the cytoarchitecture images from 1.5 to 15.0 at a reconstruction speed of 25 Hz for 1800 × 1800 pixel images. The CECEP network is widely applicable to images of different quality, different types of tissues, and different multicolor fluorescence microscopy. In addition, the CECEP network can also facilitate various downstream analysis tasks, such as cell recognition, structure tensor calculation, and brain region segmentation. With the CECEP network, we simultaneously acquired two specific fluorescence-labeled neuronal distributions and their colocated high-SBR cytoarchitecture images without crosstalk throughout the brain. Experimental results demonstrate that our method could potentially facilitate multicolor fluorescence imaging applications in biology, such as revealing and visualizing different types of biological structures with precise locations and orientations.
在多色荧光显微镜中,根据细胞结构图像的精确解剖注释,以单细胞分辨率确定生物结构的方向至关重要。然而,在同步多色成像过程中,由于光谱混合,4′,6-二脒基-2-苯基吲哚(DAPI)染色的细胞结构图像的蓝色信号串扰到绿色波段,阻碍了绿色信号的可视化和识别。在此,我们提出了一个基于深度学习的框架,名为 "串扰消除和细胞结构增强管道(CECEP)",用于在多色荧光成像过程中同时获取绿色通道中的无串扰信号和高对比度的 DAPI 染色细胞结构图像。针对 CECEP 网络,我们提出了一种名为 "细胞结构增强网络(CENet)"的无监督学习算法,该算法能在 25 Hz 的重建速度下将 1800 × 1800 像素图像的细胞结构信噪比(SBR)从 1.5 提高到 15.0。CECEP 网络广泛适用于不同质量的图像、不同类型的组织和不同的多色荧光显微镜。此外,CECEP 网络还能促进各种下游分析任务,如细胞识别、结构张量计算和脑区分割。利用 CECEP 网络,我们同时获取了两个特定的荧光标记神经元分布及其共定位的高 SBR 细胞结构图像,整个大脑中没有出现串扰。实验结果表明,我们的方法有可能促进多色荧光成像在生物学中的应用,如揭示和可视化具有精确位置和方向的不同类型的生物结构。
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引用次数: 0
778.1 nm distributed feedback lasers for Rb two-photon atomic systems with sub-4 kHz linewidths 用于掺镱双光子原子系统的 778.1 nm 分布式反馈激光器,线宽低于 4 kHz
IF 5.6 1区 物理与天体物理 Q1 OPTICS Pub Date : 2024-05-30 DOI: 10.1063/5.0191088
E. Di Gaetano, B. Keliehor, K. Gallacher, P. F. Griffin, M. Sorel, E. Riis, D. J. Paul
A new epitaxial layer design with a double mode expander layer, high refractive index claddings, and an aluminum-free active area has been used to demonstrate distributed feedback lasers operating at 778.1 nm wavelength with reduced Lorentzian linewidth aimed at miniature atomic clock applications. The design also reduces the vertical beam divergence to improve the modal matching with optical fibers as well as maintain the high power output and reduce the emission linewidth. The lasers demonstrate single-mode operation with an over 35 dB side-mode suppression ratio, a power output ≤58 mW, a coupling efficiency to tapered fibers ≤40%, and a Lorentzian linewidth of 3.7 kHz. The performance allowed the free-running distributed feedback lasers to demonstrate spectroscopy of Rb vapor, which resolved the 85Rb and 87Rb two-photon transitions.
新型外延层设计采用了双模扩展层、高折射率包层和无铝有源区,用于演示波长为 778.1 nm 的分布式反馈激光器,该激光器的洛伦兹线宽较小,主要用于微型原子钟应用。该设计还减少了垂直光束发散,从而改善了与光纤的模态匹配,并保持了高功率输出和降低了发射线宽。激光器实现了单模运行,侧模抑制比超过 35 dB,输出功率≤58 mW,与锥形光纤的耦合效率≤40%,洛伦兹线宽为 3.7 kHz。这种性能使自由运行的分布式反馈激光器能够演示掺铒蒸气的光谱分析,解析 85Rb 和 87Rb 双光子跃迁。
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引用次数: 0
Solar lasers: Why not? 太阳能激光器:为什么不呢?
IF 5.6 1区 物理与天体物理 Q1 OPTICS Pub Date : 2024-05-28 DOI: 10.1063/5.0209355
Michael Küblböck, Jonathan Will, Hanieh Fattahi
In this paper, we investigate the role of solar laser technology as a pivotal element in advancing sustainable and renewable energy. We begin by examining its wide-ranging applications across diverse fields, including remote communication, energy storage through magnesium production, and space exploration and communication. We address the current challenges faced by solar laser technology, which include the necessity for miniaturization, operation at natural sunlight intensity without the need for concentrated power, and efficient energy conversion. These improvements are essential to elevate their operational performance, beam quality, and cost-effectiveness. The promising prospects of space-based solar-pumped lasers and their potential role in magnesium generation for a sustainable energy future highlight some of the vast application opportunities that this novel technology could offer.
在本文中,我们将探讨太阳能激光技术作为推动可持续和可再生能源发展的关键因素所发挥的作用。我们首先探讨了太阳能激光技术在不同领域的广泛应用,包括远程通信、通过镁生产实现能源储存以及太空探索和通信。我们探讨了太阳能激光技术目前面临的挑战,包括微型化的必要性、在自然光照强度下运行而无需集中供电以及高效的能量转换。这些改进对于提高其运行性能、光束质量和成本效益至关重要。天基太阳能泵浦激光器的广阔前景及其在为未来可持续能源生产镁方面的潜在作用,凸显了这项新技术可能提供的一些广阔应用机会。
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引用次数: 0
Second harmonic of higher-order Poincaré sphere beam with two orthogonal 5%MgO:PPLN crystals 带有两个正交 5%MgO:PPLN 晶体的高阶波恩卡莱球形光束的二次谐波
IF 5.6 1区 物理与天体物理 Q1 OPTICS Pub Date : 2024-05-28 DOI: 10.1063/5.0198012
Qinan Jiang, Minglin Zhao, Yuanxiang Wang, Shuolin Wang, Jiantai Dou, Jun Liu, Bo Li, Youyou Hu
In this work, the second harmonic (SH) of higher-order Poincaré sphere (HOPS) beam was introduced and demonstrated with two orthogonal 5%MgO:PPLN crystals. Based on the quasi-phase-matching technique, the vectorial coupled wave equations were derived to simulate the SH of HOPS beams through the two crystals, including the cylindrical vector beams (CVBs), elliptically polarized CVBs (EPCVBs), and circularly polarized vortex beams. Then, the experimental setup was established to reveal that the SH of CVBs and EPCVBs present the four-lobed structure and still exhibit vector characteristics. Meanwhile, the circularly polarized vortex beams become the linearly polarized vortex beams with double phase topology, confirming the conservation of orbital angular momentum. Moreover, the maximum SH conversion efficiency of CVBs, EPCVBs, and circularly polarized vortex beams can reach 25.3%, 23.4%, and 29.4%, respectively, which may be instructive for promoting the SH generation of vector vortex beams with high efficiency.
这项研究介绍了高阶波恩卡莱球(HOPS)光束的二次谐波(SH),并利用两个正交的 5%MgO:PPLN 晶体进行了演示。基于准相位匹配技术,推导出矢量耦合波方程来模拟 HOPS 光束穿过两个晶体的 SH,包括圆柱矢量光束(CVB)、椭圆偏振 CVB(EPCVB)和圆偏振涡旋光束。然后,通过建立实验装置,发现 CVB 和 EPCVB 的 SH 呈现四叶结构,并仍然表现出矢量特性。同时,圆极化涡束变成了具有双相拓扑结构的线性极化涡束,证实了轨道角动量守恒。此外,CVBs、EPCVBs和圆极化涡束的最大SH转换效率分别可达25.3%、23.4%和29.4%,这对促进高效矢量涡束的SH生成可能具有指导意义。
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引用次数: 0
Mid-infrared optical coherence tomography with MHz axial line rate for real-time non-destructive testing 用于实时无损检测的兆赫轴向线速率中红外光相干断层成像技术
IF 5.6 1区 物理与天体物理 Q1 OPTICS Pub Date : 2024-05-17 DOI: 10.1063/5.0202019
Satoko Yagi, Takuma Nakamura, Kazuki Hashimoto, Shotaro Kawano, Takuro Ideguchi
Non-destructive testing (NDT) is crucial for ensuring product quality and safety across various industries. Conventional methods, such as ultrasonic, terahertz, and x-ray imaging, have limitations in terms of probe-contact requirement, depth resolution, or radiation risks. Optical coherence tomography (OCT) is a promising alternative to solve these limitations, but it suffers from strong scattering, limiting its penetration depth. Recently, OCT in the mid-infrared (MIR) spectral region has attracted attention with a significantly lower scattering rate than in the near-infrared region. However, the highest reported A-scan rate of MIR-OCT has been 3 kHz, which requires long data acquisition time to take an image, unsatisfying industrial demands for real-time diagnosis. Here, we present a high-speed MIR-OCT system operating in the 3–4 µm region that employs the frequency-swept spectrum detection in OCT technique based on time-stretch infrared spectroscopy. By integrating a broadband femtosecond MIR pulsed laser operating at a repetition rate of 50 MHz, we achieved an A-scan rate of 1 MHz with an axial resolution of 11.6 µm, a 10 dB roll-off depth of about 700 µm, and a sensitivity of 55 dB. As a proof-of-concept demonstration, we imaged the surface of substrates covered by highly scattering paint coatings. The demonstrated A-scan rate surpasses previous state of the art by more than two orders of magnitude, paving the way for real-time NDT of industrial products, cultural assets, and structures.
无损检测(NDT)对于确保各行各业的产品质量和安全至关重要。超声波、太赫兹和 X 射线成像等传统方法在探头接触要求、深度分辨率或辐射风险方面存在局限性。光学相干断层扫描(OCT)是解决这些局限性的一个很有前途的替代方法,但它的散射很强,限制了其穿透深度。最近,中红外(MIR)光谱区域的光学相干断层扫描技术引起了人们的关注,因为它的散射率明显低于近红外区域。然而,目前报道的 MIR-OCT 最高 A 扫描速率为 3 kHz,这就需要较长的数据采集时间来获取图像,无法满足实时诊断的工业需求。在此,我们提出了一种工作在 3-4 µm 区域的高速 MIR-OCT 系统,该系统在基于时间拉伸红外光谱学的 OCT 技术中采用了频扫光谱检测技术。通过集成一个以 50 MHz 重复频率工作的宽带飞秒 MIR 脉冲激光器,我们实现了 1 MHz 的 A 扫描频率,轴向分辨率为 11.6 µm,10 dB 滚降深度约为 700 µm,灵敏度为 55 dB。作为概念验证演示,我们对被高散射涂料覆盖的基底表面进行了成像。所演示的 A 扫描速率比以前的技术水平高出两个数量级以上,为工业产品、文化资产和结构的实时无损检测铺平了道路。
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引用次数: 0
HISOL: High-energy soliton dynamics enable ultrafast far-ultraviolet laser sources HISOL:高能孤子动力学实现超快远紫外激光源
IF 5.6 1区 物理与天体物理 Q1 OPTICS Pub Date : 2024-05-13 DOI: 10.1063/5.0206108
Christian Brahms, John C. Travers
Ultrafast laser sources in the far ultraviolet (100–300 nm) have been the subject of intense experimental efforts for several decades, driven primarily by the requirements of advanced experiments in ultrafast science. Resonant dispersive wave emission from high-energy laser pulses undergoing soliton self-compression in a gas-filled hollow capillary fiber promises to meet several of these requirements for the first time, most importantly by combining wide-ranging wavelength tuneability with the generation of extremely short pulses. In this Perspective, we give an overview of this approach to ultrafast far-ultraviolet sources, including its historical origin and underlying physical mechanism, the state of the art and current challenges, and our view of potential applications both within and beyond ultrafast science.
几十年来,远紫外(100-300 nm)的超快激光源一直是实验研究的热点,这主要是受超快科学先进实验要求的驱动。高能激光脉冲在充满气体的中空毛细管光纤中进行孤子自压缩时产生的共振色散波发射有望首次满足上述几项要求,其中最重要的是,它将大范围波长可调谐性与产生极短脉冲相结合。在本《视角》中,我们将概述这种超快远紫外光源的方法,包括其历史渊源和基本物理机制、技术现状和当前挑战,以及我们对超快科学内外潜在应用的看法。
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引用次数: 0
Double harmonic mode-locking in soliton fiber ring laser acquired through the resonant optoacoustic coupling 通过谐振光声耦合获得孤子光纤环形激光器中的双谐波锁模
IF 5.6 1区 物理与天体物理 Q1 OPTICS Pub Date : 2024-05-13 DOI: 10.1063/5.0195623
V. A. Ribenek, P. A. Itrin, D. A. Korobko, A. A. Fotiadi
Passive harmonic mode-locking of a soliton fiber laser locked to optoacoustic resonance (OAR) in the cavity fiber ensures high-frequency laser operation, high pulse stability, and low timing jitter. However, the pulse repetition rate (PRR) of such lasers is limited to ∼1 GHz for standard fibers due to the available acoustic modes. Here, we address these limitations by demonstrating a soliton fiber laser built from standard fiber components and subjected to double harmonic mode-locking (DHML). As an example, the laser adjusted to operate at the 15th harmonic of its cavity matching the OAR at ∼199 MHz could be driven to operate at a high harmonic of this particular OAR frequency, thus reaching ∼12 GHz. This breakthrough is made possible through controllable optoacoustic interactions in a short, 50 cm segment of unjacketed cavity fiber. We propose that the precise alignment of the laser cavity harmonic and fiber acoustic modes leads to a long-lived narrow-band acoustic vibration. This vibration sets the pace for the pulses circulating in the cavity by suppressing modes that do not conform to the Vernier principle. The surviving modes, equally spaced by the OAR frequency, in cooperation with the gain depletion and recovery mechanism, facilitate the formation of stable high-frequency pulse sequences, enabling DHML. In this process, the OAR rather than the laser cavity defines the elementary step for laser PRR tuning. Throughout the entire PRR tuning range, the soliton fiber laser exhibits enhanced stability, demonstrating supermode suppression levels better than ∼40 dB and picosecond pulse timing jitter.
孤子光纤激光器的被动谐波锁模锁定腔光纤中的光声共振(OAR),可确保激光器的高频率运行、高脉冲稳定性和低定时抖动。然而,由于可用声学模式的限制,这种激光器的脉冲重复率(PRR)在标准光纤中只能达到 ∼ 1 GHz。在此,我们展示了一种由标准光纤元件制成的孤子光纤激光器,并对其进行了双谐波模式锁定(DHML),从而解决了这些限制。举例来说,将激光器调整为在与频率为 199 MHz 的 OAR 相匹配的腔体的第 15 次谐波下工作,就能驱动激光器在这一特定 OAR 频率的高次谐波下工作,从而使频率达到 12 GHz。这一突破是在一段 50 厘米短的无套管空腔光纤中通过可控光声相互作用实现的。我们提出,激光腔谐波和光纤声学模式的精确对准导致了长寿命的窄带声学振动。这种振动通过抑制不符合维尼尔原理的模式,为在腔体内循环的脉冲设定了节奏。与 OAR 频率间隔相等的幸存模式与增益损耗和恢复机制合作,促进了稳定的高频脉冲序列的形成,从而实现了 DHML。在这个过程中,OAR 而不是激光腔决定了激光 PRR 调谐的基本步骤。在整个 PRR 调谐范围内,孤子光纤激光器表现出更高的稳定性,超模抑制水平优于 ∼ 40 dB,脉冲定时抖动为皮秒级。
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引用次数: 0
Chip-scale all-optical complex-valued matrix inverter 芯片级全光学复值矩阵反相器
IF 5.6 1区 物理与天体物理 Q1 OPTICS Pub Date : 2024-05-13 DOI: 10.1063/5.0200149
Xinyu Liu, Junwei Cheng, Hailong Zhou, Jianji Dong, Xinliang Zhang
Matrix inversion is a fundamental and widely utilized linear algebraic operation but computationally expensive in digital-clock-based platforms. Optical computing is a new computing paradigm with high speed and energy efficiency, and the computation can be realized through light propagation. However, there is a scarcity of experimentally implemented matrix inverters that exhibit both high integration density and the capability to perform complex-valued operations in existing optical systems. For the first time, we experimentally demonstrated an iterative all-optical chip-scale processor to perform the computation of complex-valued matrix inversion using the Richardson method. Our chip-scale processor achieves an iteration speed of 10 GHz, which can facilitate ultra-fast matrix inversion with the assistance of high-speed Mach–Zehnder interferometer modulators. The convergence can be attained within 20 iterations, yielding an accuracy of 90%. The proposed chip-scale all-optical complex-valued matrix inverter represents a distinctive innovation in the field of all-optical recursive systems, offering significant potential for solving computationally intensive mathematical problems.
矩阵反演是一种基本的线性代数运算,应用广泛,但在基于数字时钟的平台上计算成本高昂。光计算是一种具有高速度和高能效的新型计算模式,可通过光传播实现计算。然而,在现有光学系统中,既能实现高集成度,又能执行复值运算的矩阵反相器却很少见。我们首次在实验中展示了一种迭代式全光学芯片级处理器,利用理查森方法执行复值矩阵反演计算。我们的芯片级处理器的迭代速度达到了 10 GHz,在高速马赫-泽恩德干涉仪调制器的辅助下,可实现超快矩阵反演。收敛可在 20 次迭代内完成,精度可达 90%。所提出的芯片级全光复值矩阵反相器是全光递归系统领域的一项独特创新,为解决计算密集型数学问题提供了巨大潜力。
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引用次数: 0
Mechanically induced optical loss mechanism due to thermal expansion coefficient mismatch in micro-cavities with all-around stressor layers 带有全方位应力层的微腔中的热膨胀系数失配导致的机械诱导光学损耗机制
IF 5.6 1区 物理与天体物理 Q1 OPTICS Pub Date : 2024-05-10 DOI: 10.1063/5.0203305
Abdelrahman Z. Al-Attili, Daniel Burt, Tasmiat Rahman, Zuo Li, Naoki Higashitarumizu, Frederic Y. Gardes, Yasuhiko Ishikawa, Shinichi Saito
Various excitation-induced loss mechanisms have been identified during the development of direct-gap semiconductor lasers. Recently, indirect-gap laser sources, particularly germanium (Ge) or GeSn based, have emerged due to silicon industry compatibility. Tensile strain is crucial for optical gain or low-threshold room-temperature operation in such media. This study investigates an excitation-induced optical loss mechanism of mechanical origin in Ge-based micro-cavities with all-around stressor layers, a popular platform for strain-engineered laser sources. Using Raman spectroscopy, photoluminescence, and simulations, we find that excitation lowers the optical gain by altering the strain profile. Heating causes Ge micro-cavities to expand within a constraining stressor layer, inducing compressive strain, which is explained by the mismatch in thermal expansion coefficients.
在开发直接间隙半导体激光器的过程中,人们发现了各种激发引起的损耗机制。最近,由于硅工业的兼容性,出现了间接间隙激光源,特别是基于锗(Ge)或硒(GeSn)的激光源。拉伸应变对于此类介质的光学增益或低阈值室温操作至关重要。本研究调查了具有全方位应力层的 Ge 基微腔中的机械源激发诱导光学损耗机制,该微腔是应变工程激光源的常用平台。利用拉曼光谱、光致发光和模拟,我们发现激励通过改变应变曲线来降低光学增益。加热会使 Ge 微腔在约束应力层内膨胀,从而产生压缩应变,这可以用热膨胀系数的不匹配来解释。
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引用次数: 0
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APL Photonics
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