Active tuning of dispersive waves in Kerr soliton combs
Kerr soliton combs operate in the anomalous group-velocity dispersion regime through the excitation of dissipative solitons. The generated bandwidth is largely dependent on the cavity dispersion, with higher-order dispersion contributing to dispersive-wave (DW) generation that allows for power enhan...
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Veröffentlicht in: | Optics letters 2022-05, Vol.47 (9), p.2234-2237 |
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creator | Okawachi, Yoshitomo Kim, Bok Young Zhao, Yun Jang, Jae K Ji, Xingchen Lipson, Michal Gaeta, Alexander L |
description | Kerr soliton combs operate in the anomalous group-velocity dispersion regime through the excitation of dissipative solitons. The generated bandwidth is largely dependent on the cavity dispersion, with higher-order dispersion contributing to dispersive-wave (DW) generation that allows for power enhancement of the comb lines at the wings of the spectrum. However, the spectral position of the DW is highly sensitive to the overall cavity dispersion, and the inevitable dimension variations that occur during the fabrication process result in deviations in the DW emission wavelength. Here, we demonstrate active tuning of the DW wavelength, enabling post-fabrication spectral shaping of the soliton spectrum. We control the DW position by introducing a wavelength-controllable avoided mode crossing through actively tuning the resonances of a silicon nitride coupled microresonator via integrated heaters. We demonstrate DW tuning over 113 nm with a spectral power that can exceed the peak soliton spectral power. In addition, our modeling reveals buildup and enhancement of the DW in the auxiliary resonator, indicating that the mode hybridization arising from the strong coupling between the two resonators is critical for DW formation. |
doi_str_mv | 10.1364/OL.456609 |
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The generated bandwidth is largely dependent on the cavity dispersion, with higher-order dispersion contributing to dispersive-wave (DW) generation that allows for power enhancement of the comb lines at the wings of the spectrum. However, the spectral position of the DW is highly sensitive to the overall cavity dispersion, and the inevitable dimension variations that occur during the fabrication process result in deviations in the DW emission wavelength. Here, we demonstrate active tuning of the DW wavelength, enabling post-fabrication spectral shaping of the soliton spectrum. We control the DW position by introducing a wavelength-controllable avoided mode crossing through actively tuning the resonances of a silicon nitride coupled microresonator via integrated heaters. We demonstrate DW tuning over 113 nm with a spectral power that can exceed the peak soliton spectral power. In addition, our modeling reveals buildup and enhancement of the DW in the auxiliary resonator, indicating that the mode hybridization arising from the strong coupling between the two resonators is critical for DW formation.</description><identifier>ISSN: 0146-9592</identifier><identifier>EISSN: 1539-4794</identifier><identifier>DOI: 10.1364/OL.456609</identifier><identifier>PMID: 35486768</identifier><language>eng</language><publisher>United States: Optical Society of America</publisher><subject>Resonators ; Silicon nitride ; Solitary waves ; Tuning ; Wave dispersion</subject><ispartof>Optics letters, 2022-05, Vol.47 (9), p.2234-2237</ispartof><rights>Copyright Optical Society of America May 1, 2022</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c3299-d5ac6ea13af057676be8797d895699fc09814d4c1a45a9fbb15f2972757a70753</citedby><cites>FETCH-LOGICAL-c3299-d5ac6ea13af057676be8797d895699fc09814d4c1a45a9fbb15f2972757a70753</cites><orcidid>0000-0001-8778-6058 ; 0000-0002-9891-6206 ; 0000-0003-3418-2730 ; 0000-0002-0284-0818 ; 0000-0001-9639-0549</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,3245,27901,27902</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/35486768$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Okawachi, Yoshitomo</creatorcontrib><creatorcontrib>Kim, Bok Young</creatorcontrib><creatorcontrib>Zhao, Yun</creatorcontrib><creatorcontrib>Jang, Jae K</creatorcontrib><creatorcontrib>Ji, Xingchen</creatorcontrib><creatorcontrib>Lipson, Michal</creatorcontrib><creatorcontrib>Gaeta, Alexander L</creatorcontrib><title>Active tuning of dispersive waves in Kerr soliton combs</title><title>Optics letters</title><addtitle>Opt Lett</addtitle><description>Kerr soliton combs operate in the anomalous group-velocity dispersion regime through the excitation of dissipative solitons. The generated bandwidth is largely dependent on the cavity dispersion, with higher-order dispersion contributing to dispersive-wave (DW) generation that allows for power enhancement of the comb lines at the wings of the spectrum. However, the spectral position of the DW is highly sensitive to the overall cavity dispersion, and the inevitable dimension variations that occur during the fabrication process result in deviations in the DW emission wavelength. Here, we demonstrate active tuning of the DW wavelength, enabling post-fabrication spectral shaping of the soliton spectrum. We control the DW position by introducing a wavelength-controllable avoided mode crossing through actively tuning the resonances of a silicon nitride coupled microresonator via integrated heaters. We demonstrate DW tuning over 113 nm with a spectral power that can exceed the peak soliton spectral power. In addition, our modeling reveals buildup and enhancement of the DW in the auxiliary resonator, indicating that the mode hybridization arising from the strong coupling between the two resonators is critical for DW formation.</description><subject>Resonators</subject><subject>Silicon nitride</subject><subject>Solitary waves</subject><subject>Tuning</subject><subject>Wave dispersion</subject><issn>0146-9592</issn><issn>1539-4794</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNpd0E1Lw0AQBuBFFFurB_-ABLzoIXU3-znHUvzCQC96DpvNRrYk2bqbVPrvTWn14GlgeHhneBG6JnhOqGAPq3zOuBAYTtCUcAopk8BO0RQTJlLgkE3QRYxrjLGQlJ6jCeVMCSnUFMmF6d3WJv3Que4z8XVSubixIe6X33prY-K65M2GkETfuN53ifFtGS_RWa2baK-Oc4Y-nh7fly9pvnp-XS7y1NAMIK24NsJqQnWNuRxPllZJkJUCLgBqg0ERVjFDNOMa6rIkvM5AZpJLLbHkdIbuDrmb4L8GG_uiddHYptGd9UMsMsFVNp7ieKS3_-jaD6Ebv9sryIApRUd1f1Am-BiDrYtNcK0Ou4LgYt9mscqLQ5ujvTkmDmVrqz_5Wx_9AcR6bI4</recordid><startdate>20220501</startdate><enddate>20220501</enddate><creator>Okawachi, Yoshitomo</creator><creator>Kim, Bok Young</creator><creator>Zhao, Yun</creator><creator>Jang, Jae K</creator><creator>Ji, Xingchen</creator><creator>Lipson, Michal</creator><creator>Gaeta, Alexander L</creator><general>Optical Society of America</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>7X8</scope><orcidid>https://orcid.org/0000-0001-8778-6058</orcidid><orcidid>https://orcid.org/0000-0002-9891-6206</orcidid><orcidid>https://orcid.org/0000-0003-3418-2730</orcidid><orcidid>https://orcid.org/0000-0002-0284-0818</orcidid><orcidid>https://orcid.org/0000-0001-9639-0549</orcidid></search><sort><creationdate>20220501</creationdate><title>Active tuning of dispersive waves in Kerr soliton combs</title><author>Okawachi, Yoshitomo ; Kim, Bok Young ; Zhao, Yun ; Jang, Jae K ; Ji, Xingchen ; Lipson, Michal ; Gaeta, Alexander L</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c3299-d5ac6ea13af057676be8797d895699fc09814d4c1a45a9fbb15f2972757a70753</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Resonators</topic><topic>Silicon nitride</topic><topic>Solitary waves</topic><topic>Tuning</topic><topic>Wave dispersion</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Okawachi, Yoshitomo</creatorcontrib><creatorcontrib>Kim, Bok Young</creatorcontrib><creatorcontrib>Zhao, Yun</creatorcontrib><creatorcontrib>Jang, Jae K</creatorcontrib><creatorcontrib>Ji, Xingchen</creatorcontrib><creatorcontrib>Lipson, Michal</creatorcontrib><creatorcontrib>Gaeta, Alexander L</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>MEDLINE - Academic</collection><jtitle>Optics letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Okawachi, Yoshitomo</au><au>Kim, Bok Young</au><au>Zhao, Yun</au><au>Jang, Jae K</au><au>Ji, Xingchen</au><au>Lipson, Michal</au><au>Gaeta, Alexander L</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Active tuning of dispersive waves in Kerr soliton combs</atitle><jtitle>Optics letters</jtitle><addtitle>Opt Lett</addtitle><date>2022-05-01</date><risdate>2022</risdate><volume>47</volume><issue>9</issue><spage>2234</spage><epage>2237</epage><pages>2234-2237</pages><issn>0146-9592</issn><eissn>1539-4794</eissn><abstract>Kerr soliton combs operate in the anomalous group-velocity dispersion regime through the excitation of dissipative solitons. The generated bandwidth is largely dependent on the cavity dispersion, with higher-order dispersion contributing to dispersive-wave (DW) generation that allows for power enhancement of the comb lines at the wings of the spectrum. However, the spectral position of the DW is highly sensitive to the overall cavity dispersion, and the inevitable dimension variations that occur during the fabrication process result in deviations in the DW emission wavelength. Here, we demonstrate active tuning of the DW wavelength, enabling post-fabrication spectral shaping of the soliton spectrum. We control the DW position by introducing a wavelength-controllable avoided mode crossing through actively tuning the resonances of a silicon nitride coupled microresonator via integrated heaters. We demonstrate DW tuning over 113 nm with a spectral power that can exceed the peak soliton spectral power. 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subjects | Resonators Silicon nitride Solitary waves Tuning Wave dispersion |
title | Active tuning of dispersive waves in Kerr soliton combs |
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