(\doibase 10.1016/j.susc.2005.12.021) [****,  ()](\doibase 10.1016/S0039-6028(99)00209-5) [****, ()](http://link.aps.org/doi/10.1103/PhysRevB.64.205407) [****,  ()](\doibase
        10.1103/PhysRevE.68.010601) [****,  ()](\doibase
        10.1051/jp1:1991114) [****, ()](http://link.aps.org/doi/10.1103/PhysRevLett.66.2348) [****, ()](https://iopscience.iop.org/article/10.1088/0305-4470/33/49/301) [****,  ()](\doibase 10.1103/PhysRevLett.69.3762) [****,  ()](http://dx.doi.org/10.1016/j.physa.2016.08.057
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[^1]: The exponents $\beta=1/3$ and $1/5$ are predictions of the one-loop renormalization group [@Villain; @LSarma]. Two-loop calculations [@Janssen], however, predict corrections where the growth exponents are slightly smaller than these values.


---
author:
- 'Miles H. Anderson'
- Romain Bouchand
- Junqiu Liu
- Wenle Weng
- |
    \
    Ewelina Obrzud
- Tobias Herr
- 'Tobias J. Kippenberg'
bibliography:
- 'biblib\_2.bib'
title: 'Photonic chip-based resonant supercontinuum '
---

**Supercontinuum generation in optical fibers is one of the most dramatic nonlinear effects discovered [@alfano_observation_1970; @ranka_visible_2000; @birks_supercontinuum_2000], allowing short pulses to be converted into multi-octave spanning coherent spectra. This process has enabled self-referencing of optical frequency combs, establishing the RF-to-optical link [@jones_carrier-envelope_2000; @udem_optical_2002]. ideally suited for optical frequency division[@xi