Soliton microcombs in X-cut LiNbO3 microresonators

Abstract Chip-scale integration of optical frequency combs, particularly soliton microcombs, enables miniaturized instrumentation for timekeeping, ranging, and spectroscopy. Although soliton microcombs have been demonstrated on various material platforms, realizing complete comb functionality on pho...

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Main Authors: Binbin Nie, Xiaomin Lv, Chen Yang, Rui Ma, Kaixuan Zhu, Ze Wang, Yanwu Liu, Zhenyu Xie, Xing Jin, Guanyu Zhang, Du Qian, Zhenyu Chen, Qiang Luo, Shuting Kang, Guowei Lv, Qihuang Gong, Fang Bo, Qi-Fan Yang
Format: Article
Language:English
Published: SpringerOpen 2025-07-01
Series:eLight
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Online Access:https://doi.org/10.1186/s43593-025-00093-x
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author Binbin Nie
Xiaomin Lv
Chen Yang
Rui Ma
Kaixuan Zhu
Ze Wang
Yanwu Liu
Zhenyu Xie
Xing Jin
Guanyu Zhang
Du Qian
Zhenyu Chen
Qiang Luo
Shuting Kang
Guowei Lv
Qihuang Gong
Fang Bo
Qi-Fan Yang
author_facet Binbin Nie
Xiaomin Lv
Chen Yang
Rui Ma
Kaixuan Zhu
Ze Wang
Yanwu Liu
Zhenyu Xie
Xing Jin
Guanyu Zhang
Du Qian
Zhenyu Chen
Qiang Luo
Shuting Kang
Guowei Lv
Qihuang Gong
Fang Bo
Qi-Fan Yang
author_sort Binbin Nie
collection DOAJ
description Abstract Chip-scale integration of optical frequency combs, particularly soliton microcombs, enables miniaturized instrumentation for timekeeping, ranging, and spectroscopy. Although soliton microcombs have been demonstrated on various material platforms, realizing complete comb functionality on photonic chips requires the co-integration of high-speed modulators and efficient frequency doublers, features that are available in a monolithic form on X-cut thin-film lithium niobate (TFLN). However, the pronounced Raman nonlinearity associated with extraordinary light in this platform has so far precluded soliton microcomb generation. Here, we report the generation of transverse-electric-polarized soliton microcombs with a 25 GHz repetition rate in high-Q microresonators on X-cut TFLN chips. By precisely orienting the racetrack microresonator relative to the optical axis, we mitigate Raman nonlinearity and enable soliton formation under continuous-wave laser pumping. Moreover, the soliton microcomb spectra are extended to 350 nm with pulsed laser pumping. This work expands the capabilities of TFLN photonics and paves the way for the monolithic integration of fast-tunable, self-referenced microcombs.
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institution Kabale University
issn 2097-1710
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publishDate 2025-07-01
publisher SpringerOpen
record_format Article
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spelling doaj-art-48bc70dc603f42da9d5f3bb462fee5032025-08-20T04:01:53ZengSpringerOpeneLight2097-17102662-86432025-07-01511910.1186/s43593-025-00093-xSoliton microcombs in X-cut LiNbO3 microresonatorsBinbin Nie0Xiaomin Lv1Chen Yang2Rui Ma3Kaixuan Zhu4Ze Wang5Yanwu Liu6Zhenyu Xie7Xing Jin8Guanyu Zhang9Du Qian10Zhenyu Chen11Qiang Luo12Shuting Kang13Guowei Lv14Qihuang Gong15Fang Bo16Qi-Fan Yang17State Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking UniversityState Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking UniversityState Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking UniversityNankai UniversityState Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking UniversityState Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking UniversityState Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking UniversityState Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking UniversityState Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking UniversityState Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking UniversityState Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking UniversityNankai UniversityState Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking UniversityNankai UniversityState Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking UniversityState Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking UniversityNankai UniversityState Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking UniversityAbstract Chip-scale integration of optical frequency combs, particularly soliton microcombs, enables miniaturized instrumentation for timekeeping, ranging, and spectroscopy. Although soliton microcombs have been demonstrated on various material platforms, realizing complete comb functionality on photonic chips requires the co-integration of high-speed modulators and efficient frequency doublers, features that are available in a monolithic form on X-cut thin-film lithium niobate (TFLN). However, the pronounced Raman nonlinearity associated with extraordinary light in this platform has so far precluded soliton microcomb generation. Here, we report the generation of transverse-electric-polarized soliton microcombs with a 25 GHz repetition rate in high-Q microresonators on X-cut TFLN chips. By precisely orienting the racetrack microresonator relative to the optical axis, we mitigate Raman nonlinearity and enable soliton formation under continuous-wave laser pumping. Moreover, the soliton microcomb spectra are extended to 350 nm with pulsed laser pumping. This work expands the capabilities of TFLN photonics and paves the way for the monolithic integration of fast-tunable, self-referenced microcombs.https://doi.org/10.1186/s43593-025-00093-xThin film lithium niobateOptical frequency combOptical microresonatorNonlinear photonics
spellingShingle Binbin Nie
Xiaomin Lv
Chen Yang
Rui Ma
Kaixuan Zhu
Ze Wang
Yanwu Liu
Zhenyu Xie
Xing Jin
Guanyu Zhang
Du Qian
Zhenyu Chen
Qiang Luo
Shuting Kang
Guowei Lv
Qihuang Gong
Fang Bo
Qi-Fan Yang
Soliton microcombs in X-cut LiNbO3 microresonators
eLight
Thin film lithium niobate
Optical frequency comb
Optical microresonator
Nonlinear photonics
title Soliton microcombs in X-cut LiNbO3 microresonators
title_full Soliton microcombs in X-cut LiNbO3 microresonators
title_fullStr Soliton microcombs in X-cut LiNbO3 microresonators
title_full_unstemmed Soliton microcombs in X-cut LiNbO3 microresonators
title_short Soliton microcombs in X-cut LiNbO3 microresonators
title_sort soliton microcombs in x cut linbo3 microresonators
topic Thin film lithium niobate
Optical frequency comb
Optical microresonator
Nonlinear photonics
url https://doi.org/10.1186/s43593-025-00093-x
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