Abstract

Nonlinear interactions within compact, on-chip microring resonant cavities is a topic of increasing interest in current silicon photonics research. Frequency combs, one of the emerging nonlinear applications in microring optics, offers great potential from both scientific and practical perspectives. However, the mechanisms of comb formation appear to differ from traditional frequency combs formed by pulsed femtosecond lasers, and thus require detailed elucidation through theory and simulation. Here we propose a technique to mimic the accuracy of finite-difference time domain (FDTD) full wave nonlinear optical simulations with only a small fraction of the computational resources. Our new hybrid approach combines a single linear FDTD simulation of the key interaction parameters, then directly inserts them into a coupled-mode theory simulation. Comparison of the hybrid approach and full FDTD shows a good match both in frequency domain and in time domain. Thus, it retains the advantage of FDTD in terms of direct connection with experimental designs, while finishing much faster and sidestepping stability issues associated with direct simulation of nonlinear phenomena. The hybrid technique produces several key results explored in this paper, including: demonstrating that comb formation can occur with both anomalous and normal dispersion; suggesting a new mechanism for incoherent (Type II) frequency comb formation; and illustrating a method for creating soliton-like pulses in on-chip microresonators.

Highlights

  • Optical frequency comb formation is a very powerful technology, in which optical narrowband signals are created at predetermined frequency intervals with precisely controlled amplitudes and phases [1]

  • In this part of the manuscript, we show that our expectations of comb generation dynamics are confirmed with direct finite-difference time domain simulation, and show the corresponding coupled-mode theory simulations that corroborate our prior observations

  • We can observe a close correlation between the finite-difference time domain (FDTD) and coupled mode theory (CMT) simulations performed using narrowband excitation, from perspectives in the time domain in Figs. 4(a), 4(b), 5(a), and 5(b), as well as perspectives in the frequency domain in Figs. 4(c), 4(d), 5(c), and 5(d)

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Summary

Introduction

Optical frequency comb formation is a very powerful technology, in which optical narrowband signals are created at predetermined frequency intervals with precisely controlled amplitudes and phases [1]. Optical combs are generated by using a pulsed femtosecond laser. Such a solution tends to be relatively bulky and expensive. With recent advances in fabrication techniques, on-chip microresonators have recently been developed [6, 7]. If these microresonators are excited by common continuous-wave (cw) pump lasers, optical frequency combs can be generated within a compact form factor [1,2,3,4,5, 8,9,10,11,12,13]. For four-wave mixing processes, a 1,000-fold increase in intensity associated with photonic mode confinement can increase signal and idler generation by a factor of 1,000,000 or more [15]

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