Topological soliton frequency comb in nanophotonic lithium niobate.
basic_science · Level V
Where this comes from
- Record sourced from PubMed, PMID 41882366.
- Also identified by DOI 10.1038/s41586-026-10292-2.
- No licence information is recorded for this record.
- Because redistribution is not established, this page shows the abstract only. Follow the links below for the full text.
Abstract
Frequency combs have revolutionized metrology, ranging and optical clocks<sup>1</sup>, motivating substantial efforts on the development of chip-scale comb sources<sup>2,3</sup>. Some on-chip comb sources exist and have been implemented through electro-optic modulation<sup>4,5</sup>, mode-locked lasers<sup>6,7</sup>, quantum cascade lasers<sup>8-10</sup> or soliton formation by Kerr nonlinearity<sup>11,12</sup>. However, widespread deployment of on-chip comb sources has remained elusive, as they still require radiofrequency sources, high-Q (high-quality factor) resonators or complex stabilization schemes while facing efficiency challenges. Here, we demonstrate an on-chip frequency comb source based on the integration of a lithium niobate nanophotonic circuit with a semiconductor laser that can alleviate these challenges. We show the formation of temporal topological solitons in an on-chip nanophotonic parametric oscillator with quadratic nonlinearity and low finesse. These solitons, independent of the dispersion regime, consist of phase defects separating two π-out-of-phase continuous wave solutions at the signal frequency, which is half the input pump frequency<sup>13,14</sup>. We use on-chip cross-correlation for temporal measurements and confirm formation of topological solitons as short as 60 fs around 2 μm, in agreement with a generalized parametrically forced Ginzburg-Landau theory<sup>15-17</sup>. Moreover, we demonstrate a proof-of-concept turn-key operation of a hybrid-integrated source of topological frequency comb. Topological solitons are potential candidates for the development of integrated comb sources, which are dispersion-sign agnostic and do not require high-Q resonators or high-speed modulators, and can provide access to hard-to-reach spectral regions, including mid-infrared regions<sup>18</sup>.