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. 2020 Jan 20;9:9. doi: 10.1038/s41377-020-0246-7

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© The Author(s) 2020

Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.

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Fig. 5 — a Kerr oscillation for the TM mode from an X-cut LN microresonator as the pump laser is red-detuned into the cavity resonance (top to bottom). b RF spectra corresponding to States (ii) and (iii) in a. c Transmission measurement of the microresonator output above 1570 nm, which excludes the pump wavelength. The laser is tuned to the resonance as the wavelength increases, dominated by the thermal-optic effect. The laser sweeping speed is 80 pm/ms. d Zoom-in of the transmission trace in c, which shows the onset of the soliton step.