pith. sign in

arxiv: 1606.00954 · v1 · pith:5UT5RVOGnew · submitted 2016-06-03 · ⚛️ physics.optics

Spatial-mode-interaction-induced dispersive-waves and their active tuning in microresonators

classification ⚛️ physics.optics
keywords dispersivewavesinteractionsgenerationopticalsolitonwavecontrol
0
0 comments X p. Extension
pith:5UT5RVOG Add to your LaTeX paper What is a Pith Number?
\usepackage{pith}
\pithnumber{5UT5RVOG}

Prints a linked pith:5UT5RVOG badge after your title and writes the identifier into PDF metadata. Compiles on arXiv with no extra files. Learn more

read the original abstract

The nonlinear propagation of optical pulses in dielectric waveguides and resonators provides a laboratory to investigate a wide range of remarkable interactions. Many of the resulting phenomena find applications in optical systems. One example is dispersive wave generation, the optical analog of Cherenkov radiation. These waves have an essential role in fiber spectral broadeners that are routinely used in spectrocopy and metrology. Dispersive waves form when a soliton pulse begins to radiate power as a result of higher-order dispersion. Recently, dispersive wave generation in microcavities has been reported by phase matching the waves to dissipative Kerr cavity (DKC) solitons. Here, it is shown that spatial mode interactions within a microcavity can also be used to induce dispersive waves. These interactions are normally avoided altogether in DKC soliton generation. The soliton self frequency shift is also shown to induce fine tuning control of the dispersive wave frequency. Both this mechanism and spatial mode interactions provide a new method to spectrally control these important waves.

This paper has not been read by Pith yet.

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.