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Soliton Bursts and Deterministic Dissipative Kerr Soliton Generation

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Soliton Bursts and Deterministic Dissipative Kerr Soliton Generation Zhou et al. Light: Science & Applications (2019) 8:50 Official journal of the CIOMP 2047-7538 https://doi.org/10.1038/s41377-019-0161-y www.nature.com/lsa ARTICLE Open Access Soliton bursts and deterministic dissipative Kerr soliton generation in auxiliary-assisted microcavities Heng Zhou1,YongGeng1,WenwenCui1,Shu-WeiHuang2,3, Qiang Zhou 4,KunQiu1 and Chee Wei Wong2 Abstract Dissipative Kerr solitons in resonant frequency combs offer a promising route for ultrafast mode-locking, precision spectroscopy and time-frequency standards. The dynamics for the dissipative soliton generation, however, are intrinsically intertwined with thermal nonlinearities, limiting the soliton generation parameter map and statistical success probabilities of the solitary state. Here, via use of an auxiliary laser heating approach to suppress thermal dragging dynamics in dissipative soliton comb formation, we demonstrate stable Kerr soliton singlet formation and soliton bursts. First, we access a new soliton existence range with an inverse-sloped Kerr soliton evolution— diminishing soliton energy with increasing pump detuning. Second, we achieve deterministic transitions from Turing- like comb patterns directly into the dissipative Kerr soliton singlet pulse bypassing the chaotic states. This is achieved by avoiding subcomb overlaps at lower pump power, with near-identical singlet soliton comb generation over twenty instances. Third, with the red-detuned pump entrance route enabled, we uncover unique spontaneous soliton bursts in the direct formation of low-noise optical frequency combs from continuum background noise. The burst dynamics are due to the rapid entry and mutual attraction of the pump laser into the cavity mode, aided by the auxiliary laser and matching well with our numerical simulations. Enabled by the auxiliary-assisted frequency comb dynamics, we 1234567890():,; 1234567890():,; 1234567890():,; 1234567890():,; demonstrate an application of automatic soliton comb recovery and long-term stabilization against strong external perturbations. Our findings hold potential to expand the parameter space for ultrafast nonlinear dynamics and precision optical frequency comb stabilization. – Introduction ultrashort mode-locked pulses4 6 and broadband comb – Dissipative Kerr solitons (DKS) can be obtained in spectra7 10 with good intrinsic stabilization potential11 optical cavities through the double balancing of cavity loss and a smooth envelope12. Moreover, DKS microcombs – with third-order nonlinear parametric amplification and not only exhibit abundant physical dynamics13 26 but also – cavity dispersion with self-phase modulation (SPM)1 3.In demonstrate immense practical prospects ranging from particular, DKS generated in high finesse microresonators high capacity fiber transmission27,28, an ultra-stable associated with a Kerr frequency comb has attracted microwave source29, and a photonic frequency synthesi- – considerable interest, as it simultaneously gives rise to zer30, to precision laser metrology and spectroscopy31 35. The robust generation of DKS, especially the single soliton state, however, remains difficult due to the sizable Correspondence: Heng Zhou ([email protected])or cavity thermal nonlinearity1,36, which prevents the pump Chee Wei Wong ([email protected]) 1Key Lab of Optical Fiber Sensing and Communication Networks, University of laser from entering the parameter space where the dual- Electronic Science and Technology of China, 611731 Chengdu, China balanced solitary waveforms exist. The current strategy 2 Fang Lu Mesoscopic Optics and Quantum Electronics Laboratory, University used for DKS formation is based on the fast scanning of of California, Los Angeles, CA 90095, USA Full list of author information is available at the end of the article. pump laser frequency to overtake the slower dragged These authors equal contribution eqally: Heng Zhou, Yong Geng © The Author(s) 2019 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 linktotheCreativeCommons 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/. Zhou et al. Light: Science & Applications (2019) 8:50 Page 2 of 10 thermal response in a rapidly changing intracavity wave- mode caused by mode-crossing with another spatial mode form and stopping the pump as close to the optimal family is observed4,12, the influence of which will be dis- – condition as possible6,15,37 41. This scheme sets the cussed in the below sections. microresonator to a delicate thermal equilibrium with Our approach uses two external cavity diode lasers complex detuning conditions of the intracavity light (ECDL), which are amplified and launched into the fields;1,15 consequently, one requires rigidly conducted microcavity from opposite directions (Fig. 1a). First, an 39–41 5,38 pump frequency-sweeping and “power kicking” , auxiliary laser (Eaux) is frequency tuned into a resonance during which precision control of the soliton state is (≈1532.8 nm in our experiment) following the traditional cumbersome38,40. Moreover, such a fast pump scanning self-thermal locking trajectory and is stopped near the approach contains an intrinsic prerequisite that, to keep resonance peak but still kept blue-detuned. Subsequently, the cavity in thermal equilibrium, the intracavity light a pump laser (Epump) is tuned into another resonance fields must sustain effective blue-detuning even after the (≈1538.8 nm) in the counter-propagating direction. Due 1,40 pump laser enters the red-detuning resonance region . to the effect of Eaux, the evolution of Epump is significantly This prerequisite results in high pump power operation modified from the conventional pathway. In particular, as and, thereby, a chaotic stage prior to accessing the low- Epump is tuned into resonance from the blue side, all the – noise soliton states42 44. The resulting DKS pulse number resonances are heated and thermally pushed to longer and its comb envelope thus vary from measurement to wavelengths, which displaces Eaux from its resident reso- measurement. Consequently, thermal compensation nance and cools the microcavity in counter-balance. approaches have been investigated, such as cavity opto- Likewise, when Epump leaves the cavity resonance from the 45 mechanics with dual lasers and stabilization of the cavity red side and cools the cavity, Eaux will re-enter its resident mode spacing46. resonance and in turn heat the cavity (see Supplementary Here, we demonstrate, via an auxiliary laser heating Information Section I). By aptly configuring the power approach, an expanded operating phase space for the and frequency for Eaux, the heat flow caused by Epump can nonlinear transitions of the Kerr frequency comb along be largely balanced out, keeping the cavity temperature with unique dynamics. Through separation of the cavity and all cavity resonances approximately unchanged. This thermal nonlinearities from the Kerr dynamics, we first allows the pump laser to be stably tuned across the entire uncover an existence range in the inverse-sloped Kerr resonance with minimized thermal behavior. Further- soliton evolution featuring a diminishing soliton energy more, since Eaux and Epump are counter-propagating light with increasing pump detuning, arising from a unique waves with different detunings, the Kerr-nonlinearity balance between soliton peak power and pulse width. cross-phase modulation (XPM) between them induces a Second, we report deterministic transitions from Turing- slowly varying nonlinear detuning offset48, which retards like comb patterns directly into a dissipative Kerr soliton the change in the effective pump detuning (similar to singlet pulse, avoiding the subcomb overlaps and thereby thermal counter-dragging) and in turn increases the bypassing the chaotic states in the formation dynamics. detuning range wherein DKS can be accessed (see Sup- Third, we illustrate dissipative Kerr soliton bursts arising plementary Information Section VIII). from background noise via the red-detuning pump As shown in Fig. 1c, by implementing a dual-driven entrance. Aided by these new findings, we implement an scheme, the experimentally measured power transmis- automatic soliton recovery algorithm against strong sions, Epump and Eaux, clearly illustrate their counter- external perturbations. balanced contributions to the cavity thermal behavior. We observe that when the pump traverses from the blue- Results detuning (λi) to the red-detuning (λiii) regime, stable Stable DKS generation via auxiliary laser heating comb spectra can be formed, as shown in Fig. 1d-(i)–d- Figure 1a illustrates our experimental setup. A Si3N4 (iii). Specifically, when the Epump is blue-detuned (λi), microring cavity with a width-height cross-section of subcombs with well separated line doublets (i.e., spacing 2000 × 800 nm2 and a loaded Q-factor of ≈500,000 is multiple FSR) are generated42,
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