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Photo-induced cascaded harmonic and comb generation in silicon nitride microresonators

Silicon nitride (Si(3)N(4)) is an ever-maturing integrated platform for nonlinear optics but mostly considered for third-order [χ((3))] nonlinear interactions. Recently, second-order [χ((2))] nonlinearity was introduced into Si(3)N(4) via the photogalvanic effect, resulting in the inscription of qua...

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Detalles Bibliográficos
Autores principales: Hu, Jianqi, Nitiss, Edgars, He, Jijun, Liu, Junqiu, Yakar, Ozan, Weng, Wenle, Kippenberg, Tobias J., Brès, Camille-Sophie
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Association for the Advancement of Science 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9750138/
https://www.ncbi.nlm.nih.gov/pubmed/36516262
http://dx.doi.org/10.1126/sciadv.add8252
Descripción
Sumario:Silicon nitride (Si(3)N(4)) is an ever-maturing integrated platform for nonlinear optics but mostly considered for third-order [χ((3))] nonlinear interactions. Recently, second-order [χ((2))] nonlinearity was introduced into Si(3)N(4) via the photogalvanic effect, resulting in the inscription of quasi-phase–matched χ((2)) gratings. However, the full potential of the photogalvanic effect in microresonators remains largely unexplored for cascaded effects. Here, we report combined χ((2)) and χ((3)) nonlinear effects in a normal dispersion Si(3)N(4) microresonator. We demonstrate that the photo-induced χ((2)) grating also provides phase-matching for the sum-frequency generation process, enabling the initiation and successive switching of primary combs. In addition, the doubly resonant pump and second-harmonic fields allow for effective third-harmonic generation, where a secondary optically written χ((2)) grating is identified. Last, we reach a broadband microcomb state evolved from the sum-frequency–coupled primary comb. These results expand the scope of cascaded effects in microresonators.