论文标题
零分散kerr soliton在光学微孔子中
Zero-dispersion Kerr solitons in optical microresonators
论文作者
论文摘要
孤子是保留在非线性动力学系统中无处不在的波形的形状,并属于两个单独的类别,即在异常组速度分散体中形成的明亮孤子,在正常分散体中形成的“暗孤子”。在BEC,流体动力学,极化子和模式锁定激光器中都观察到了两种类型的孤子,但与许多系统水平应用中的基于碎屑微孔子的频率梳(Microcombs)的生成特别相关,这些频率梳子(Microcombs)在时间级应用中使用。对于微型小子,已经研究了明亮的孤子和基于互锁开关波的深色脉冲。然而,理论上已经预测了适合这种二分法之间的局部耗散结构的存在,但在实验上难以捉摸。在这里,我们报告了在开关波和耗散孤子之间体现杂种的耗散结构的发现,这些结构存在于(几乎)消失的组速度分散体的状态下,其中三阶分散占主导地位,因此被称为“零分散孤子子”。这些耗散结构是通过塌陷的开关波形成形成的,形成了量化的孤子子结构的簇。开关波是通过基于光子芯片的SI3N4微孔子的同步脉冲驾驶直接形成的。在开关波和零分散的孤子状态下,所得的频率频谱都非常宽,达到136 THz或八度的97%。四阶分散工程会导致双分散性波的形成,并与法拉第不稳定性相关的新型准阶段匹配。这种异国情调的意外耗散结构将Kerr腔物理学的结构域扩展到零分散附近的制度,并可能为宽带梳子发电提供了一种较优质的替代方案。
Solitons are shape preserving waveforms that are ubiquitous across nonlinear dynamical systems and fall into two separate classes, that of bright solitons, formed in the anomalous group velocity dispersion regime, and `dark solitons' in the normal dispersion regime. Both types of soliton have been observed in BEC, hydrodynamics, polaritons, and mode locked lasers, but have been particularly relevant to the generation of chipscale microresonator-based frequency combs (microcombs), used in numerous system level applications in timing, spectroscopy, and communications. For microcombs, both bright solitons, and alternatively dark pulses based on interlocking switching waves, have been studied. Yet, the existence of localized dissipative structures that fit between this dichotomy has been theoretically predicted, but proven experimentally elusive. Here we report the discovery of dissipative structures that embody a hybrid between switching waves and dissipative solitons, existing in the regime of (nearly) vanishing group velocity dispersion where third-order dispersion is dominant, hence termed as `zero-dispersion solitons'. These dissipative structures are formed via collapsing switching wave fronts, forming clusters of quantized solitonic sub-structures. The switching waves are formed directly via synchronous pulse-driving of a photonic chip-based Si3N4 microresonator. The resulting frequency comb spectrum is extremely broad in both the switching wave and zero-dispersion soliton regime, reaching 136 THz or 97% of an octave. Fourth-order dispersion engineering results in dual-dispersive wave formation, and a novel quasi-phase matched wave related to Faraday instability. This exotic unanticipated dissipative structure expands the domain of Kerr cavity physics to the regime near zero-dispersion and could present a superior alternative to conventional solitons for broadband comb generation.