Abstract

Mode-coupling-induced dispersion has been used to engineer microresonators for soliton generation at the edge of the visible band. Here, we show that the optical soliton formed in this way is analogous to optical Bragg solitons and, more generally, to the Dirac soliton in quantum field theory. This optical Dirac soliton is studied theoretically, and a closed-form solution is derived in the corresponding conservative system. Both analytical and numerical solutions show unusual properties, such as polarization twisting and asymmetrical optical spectra. The closed-form solution is also used to study the repetition rate shift in the soliton. An observation of the asymmetrical spectrum is analysed using theory. The properties of Dirac optical solitons in microresonators are important at a fundamental level and provide a road map for soliton microcomb generation in the visible band.

Highlights

  • Soliton mode locking in microresonators[1] provides a pathway for the miniaturization of frequency comb systems[2]

  • The resulting hyperbolic shape of the eigenfrequency dispersion creates an anomalous dispersion window that is suitable for soliton generation

  • The curvature of a circular resonator contributes to normal dispersion, shifting the zero-dispersion wavelength towards longer wavelengths as the resonator size decreases

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Summary

Introduction

Soliton mode locking in microresonators[1] provides a pathway for the miniaturization of frequency comb systems[2]. Wherein distinct mode families experience frequency degeneracy analogous to an energy level crossing[29], is an important feature of soliton formation in microresonators Such crossings impart structure to the soliton spectral envelope[30] and are responsible for an intriguing range of microcomb phenomena of both scientific and technical importance, including dispersive wave emissions[9,31], dark soliton formation[32], pump noise isolation[33], improved pumping efficiency[34,35], and dispersion engineering for near-visible emissions[36,37]

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