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用于单模和多模光子学的具有任意功率比的1×集成功率分配器的制造。

Fabrication of 1 × integrated power splitters with arbitrary power ratio for single and multimode photonics.

作者信息

Haines Jack, Vitali Valerio, Bottrill Kyle, Naik Pooja Uday, Gandolfi Marco, De Angelis Costantino, Franz Yohann, Lacava Cosimo, Petropoulos Periklis, Guasoni Massimiliano

机构信息

Optoelectronics Research Centre, University of Southampton, Southampton, England.

Department of Electrical, Computer and Biomedical Engineering, University of Pavia, Pavia, Italy.

出版信息

Nanophotonics. 2024 Jan 24;13(3):339-348. doi: 10.1515/nanoph-2023-0694. eCollection 2024 Feb.

DOI:10.1515/nanoph-2023-0694
PMID:39633675
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11501587/
Abstract

Compact power splitters are essential components in integrated optics. While 1 × 2 power splitters with uniform splitting are widely used, a 1 × splitter with arbitrary number of ports and arbitrary splitting ratio is yet to be demonstrated. In this work we address this problem. We fabricate and characterise 1 × integrated power splitters that provide fully arbitrary splitting ratios. The core of our design is represented by an array of non-equally spaced waveguides fabricated on a silicon nitride-on-insulator wafer. Any arbitrary 1 × splitting ratio can be achieved by properly setting the array length and the dimension of the (-1) nano-gaps between the adjacent waveguides. Most importantly, at variance with state-of-the-art solutions, our devices can be designed for arbitrary splitting of higher-order modes. In this manuscript we provide the first experimental demonstration of 1 × arbitrary splitting ratio for both the fundamental modes (TE00 and TM00) and the TE01 mode, here up to = 5 ports. With a footprint of 20 μm/port, a bandwidth up to 70 nm and an excess losses <0.2 dB, our devices set a new benchmark for optical power splitters in both standard single-mode photonics as well as in the emerging integrated multimode photonics technology, and may therefore boost key photonic applications, from optimal power distribution and equalization up to signal processing operations.

摘要

紧凑型功率分配器是集成光学中的关键组件。虽然具有均匀分光的1×2功率分配器被广泛使用,但具有任意端口数量和任意分光比的1×N功率分配器尚未得到验证。在这项工作中,我们解决了这个问题。我们制造并表征了能提供完全任意分光比的1×N集成功率分配器。我们设计的核心是由在绝缘体上氮化硅晶圆上制造的一系列非等距波导组成。通过适当设置阵列长度和相邻波导之间(-1)纳米间隙的尺寸,可以实现任何任意的1×N分光比。最重要的是,与现有技术的解决方案不同,我们的器件可以设计用于高阶模式的任意分光。在本手稿中,我们首次对基模(TE00和TM00)以及TE01模式进行了1×N任意分光比的实验验证,此处N可达5个端口。我们的器件每端口占地面积为20μm,带宽高达70nm,额外损耗<0.2dB,在标准单模光子学以及新兴的集成多模光子学技术中,为光功率分配器树立了新的标杆,因此可能会推动关键的光子应用,从最优功率分配和均衡到信号处理操作。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0d45/11501587/f66ec6c6bb8a/j_nanoph-2023-0694_fig_007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0d45/11501587/e5897a1baf8d/j_nanoph-2023-0694_fig_001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0d45/11501587/bccabd8955ef/j_nanoph-2023-0694_fig_002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0d45/11501587/acb3620d5c53/j_nanoph-2023-0694_fig_003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0d45/11501587/810558c3c239/j_nanoph-2023-0694_fig_004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0d45/11501587/a31029241f1f/j_nanoph-2023-0694_fig_005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0d45/11501587/b38d9f3c1aa0/j_nanoph-2023-0694_fig_006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0d45/11501587/f66ec6c6bb8a/j_nanoph-2023-0694_fig_007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0d45/11501587/e5897a1baf8d/j_nanoph-2023-0694_fig_001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0d45/11501587/bccabd8955ef/j_nanoph-2023-0694_fig_002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0d45/11501587/acb3620d5c53/j_nanoph-2023-0694_fig_003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0d45/11501587/810558c3c239/j_nanoph-2023-0694_fig_004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0d45/11501587/a31029241f1f/j_nanoph-2023-0694_fig_005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0d45/11501587/b38d9f3c1aa0/j_nanoph-2023-0694_fig_006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0d45/11501587/f66ec6c6bb8a/j_nanoph-2023-0694_fig_007.jpg

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