Anderson Miles H, Weng Wenle, Lihachev Grigory, Tikan Alexey, Liu Junqiu, Kippenberg Tobias J
Institute of Physics, Swiss Federal Institute of Technology Lausanne (EPFL), 1015, Lausanne, Switzerland.
Institute for Photonics and Advanced Sensing (IPAS), and School of Physical Sciences, The University of Adelaide, Adelaide, SA, 5005, Australia.
Nat Commun. 2022 Aug 13;13(1):4764. doi: 10.1038/s41467-022-31916-x.
Solitons are shape preserving waveforms that are ubiquitous across nonlinear dynamical systems from BEC to hydrodynamics, and fall into two separate classes: bright solitons existing in anomalous group velocity dispersion, and switching waves forming 'dark solitons' in normal dispersion. Bright solitons in particular have been relevant to chip-scale microresonator frequency combs, used in applications across communications, metrology, and spectroscopy. Both have been studied, yet the existence of a structure between this dichotomy has only been theoretically predicted. We report the observation of dissipative structures embodying a hybrid between switching waves and dissipative solitons, existing in the regime of vanishing group velocity dispersion where third-order dispersion is dominant, hence termed as 'zero-dispersion solitons'. They are observed to arise from the interlocking of two modulated switching waves, forming a stable solitary structure consisting of a quantized number of peaks. The switching waves form directly via synchronous pulse-driving of a SiN microresonator. The resulting comb spectrum spans 136 THz or 97% of an octave, further enhanced by higher-order dispersive wave formation. This dissipative structure expands the domain of Kerr cavity physics to the regime near to zero-dispersion and could present a superior alternative to conventional solitons for broadband comb generation.
孤子是一种形状保持波形,在从玻色-爱因斯坦凝聚到流体动力学的非线性动力系统中普遍存在,可分为两类:存在于反常群速度色散中的亮孤子,以及在正常色散中形成“暗孤子”的开关波。特别是亮孤子与芯片级微谐振器频率梳相关,应用于通信、计量学和光谱学等领域。这两类孤子都已被研究过,但在这种二分法之间存在一种结构的情况仅在理论上被预测过。我们报告了对一种耗散结构的观测,该结构体现了开关波和耗散孤子之间的混合,存在于群速度色散消失且三阶色散占主导的区域,因此被称为“零色散孤子”。观察到它们由两个调制开关波的联锁产生,形成一个由量化数量的峰值组成的稳定孤立结构。开关波通过对氮化硅微谐振器的同步脉冲驱动直接形成。由此产生的梳状频谱跨度为136太赫兹或一个倍频程的97%,通过高阶色散波的形成进一步增强。这种耗散结构将克尔腔物理领域扩展到接近零色散的区域,并且可能为宽带梳状生成提供一种优于传统孤子的替代方案。