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Zero dispersion Kerr solitons in optical microresonators
Solitons are shape preserving waveforms that are ubiquitous across nonlinear dynamical systems from BEC to hydrodynamics, and fall into two separate classes: bright solitons existing in anomalous group velocity dispersion, and switching waves forming ‘dark solitons’ in normal dispersion. Bright soli...
Autores principales: | , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9376110/ https://www.ncbi.nlm.nih.gov/pubmed/35963859 http://dx.doi.org/10.1038/s41467-022-31916-x |
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author | Anderson, Miles H. Weng, Wenle Lihachev, Grigory Tikan, Alexey Liu, Junqiu Kippenberg, Tobias J. |
author_facet | Anderson, Miles H. Weng, Wenle Lihachev, Grigory Tikan, Alexey Liu, Junqiu Kippenberg, Tobias J. |
author_sort | Anderson, Miles H. |
collection | PubMed |
description | Solitons are shape preserving waveforms that are ubiquitous across nonlinear dynamical systems from BEC to hydrodynamics, and fall into two separate classes: bright solitons existing in anomalous group velocity dispersion, and switching waves forming ‘dark solitons’ in normal dispersion. Bright solitons in particular have been relevant to chip-scale microresonator frequency combs, used in applications across communications, metrology, and spectroscopy. Both have been studied, yet the existence of a structure between this dichotomy has only been theoretically predicted. We report the observation of dissipative structures embodying a hybrid between switching waves and dissipative solitons, existing in the regime of vanishing group velocity dispersion where third-order dispersion is dominant, hence termed as ‘zero-dispersion solitons’. They are observed to arise from the interlocking of two modulated switching waves, forming a stable solitary structure consisting of a quantized number of peaks. The switching waves form directly via synchronous pulse-driving of a Si(3)N(4) microresonator. The resulting comb spectrum spans 136 THz or 97% of an octave, further enhanced by higher-order dispersive wave formation. This dissipative structure expands the domain of Kerr cavity physics to the regime near to zero-dispersion and could present a superior alternative to conventional solitons for broadband comb generation. |
format | Online Article Text |
id | pubmed-9376110 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-93761102022-08-15 Zero dispersion Kerr solitons in optical microresonators Anderson, Miles H. Weng, Wenle Lihachev, Grigory Tikan, Alexey Liu, Junqiu Kippenberg, Tobias J. Nat Commun Article Solitons are shape preserving waveforms that are ubiquitous across nonlinear dynamical systems from BEC to hydrodynamics, and fall into two separate classes: bright solitons existing in anomalous group velocity dispersion, and switching waves forming ‘dark solitons’ in normal dispersion. Bright solitons in particular have been relevant to chip-scale microresonator frequency combs, used in applications across communications, metrology, and spectroscopy. Both have been studied, yet the existence of a structure between this dichotomy has only been theoretically predicted. We report the observation of dissipative structures embodying a hybrid between switching waves and dissipative solitons, existing in the regime of vanishing group velocity dispersion where third-order dispersion is dominant, hence termed as ‘zero-dispersion solitons’. They are observed to arise from the interlocking of two modulated switching waves, forming a stable solitary structure consisting of a quantized number of peaks. The switching waves form directly via synchronous pulse-driving of a Si(3)N(4) microresonator. The resulting comb spectrum spans 136 THz or 97% of an octave, further enhanced by higher-order dispersive wave formation. This dissipative structure expands the domain of Kerr cavity physics to the regime near to zero-dispersion and could present a superior alternative to conventional solitons for broadband comb generation. Nature Publishing Group UK 2022-08-13 /pmc/articles/PMC9376110/ /pubmed/35963859 http://dx.doi.org/10.1038/s41467-022-31916-x Text en © The Author(s) 2022 https://creativecommons.org/licenses/by/4.0/Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) . |
spellingShingle | Article Anderson, Miles H. Weng, Wenle Lihachev, Grigory Tikan, Alexey Liu, Junqiu Kippenberg, Tobias J. Zero dispersion Kerr solitons in optical microresonators |
title | Zero dispersion Kerr solitons in optical microresonators |
title_full | Zero dispersion Kerr solitons in optical microresonators |
title_fullStr | Zero dispersion Kerr solitons in optical microresonators |
title_full_unstemmed | Zero dispersion Kerr solitons in optical microresonators |
title_short | Zero dispersion Kerr solitons in optical microresonators |
title_sort | zero dispersion kerr solitons in optical microresonators |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9376110/ https://www.ncbi.nlm.nih.gov/pubmed/35963859 http://dx.doi.org/10.1038/s41467-022-31916-x |
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