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Optoelectronic parametric oscillator
Oscillators are one of the key elements in various applications as a signal source to generate periodic oscillations. Among them, an optical parametric oscillator (OPO) is a driven harmonic oscillator based on parametric frequency conversion in an optical cavity, which has been widely investigated a...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
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Nature Publishing Group UK
2020
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7295800/ https://www.ncbi.nlm.nih.gov/pubmed/32566172 http://dx.doi.org/10.1038/s41377-020-0337-5 |
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author | Hao, Tengfei Cen, Qizhuang Guan, Shanhong Li, Wei Dai, Yitang Zhu, Ninghua Li, Ming |
author_facet | Hao, Tengfei Cen, Qizhuang Guan, Shanhong Li, Wei Dai, Yitang Zhu, Ninghua Li, Ming |
author_sort | Hao, Tengfei |
collection | PubMed |
description | Oscillators are one of the key elements in various applications as a signal source to generate periodic oscillations. Among them, an optical parametric oscillator (OPO) is a driven harmonic oscillator based on parametric frequency conversion in an optical cavity, which has been widely investigated as a coherent light source with an extremely wide wavelength tuning range. However, steady oscillation in an OPO is confined by the cavity delay, which leads to difficulty in frequency tuning, and the frequency tuning is discrete with the minimum tuning step determined by the cavity delay. Here, we propose and demonstrate a counterpart of an OPO in the optoelectronic domain, i.e., an optoelectronic parametric oscillator (OEPO) based on parametric frequency conversion in an optoelectronic cavity to generate microwave signals. Owing to the unique energy-transition process in the optoelectronic cavity, the phase evolution in the OEPO is not linear, leading to steady single-mode oscillation or multimode oscillation that is not bounded by the cavity delay. Furthermore, the multimode oscillation in the OEPO is stable and easy to realize owing to the phase control of the parametric frequency-conversion process in the optoelectronic cavity, while stable multimode oscillation is difficult to achieve in conventional oscillators such as an optoelectronic oscillator (OEO) or an OPO due to the mode-hopping and mode-competition effect. The proposed OEPO has great potential in applications such as microwave signal generation, oscillator-based computation, and radio-frequency phase-stable transfer. |
format | Online Article Text |
id | pubmed-7295800 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2020 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-72958002020-06-19 Optoelectronic parametric oscillator Hao, Tengfei Cen, Qizhuang Guan, Shanhong Li, Wei Dai, Yitang Zhu, Ninghua Li, Ming Light Sci Appl Article Oscillators are one of the key elements in various applications as a signal source to generate periodic oscillations. Among them, an optical parametric oscillator (OPO) is a driven harmonic oscillator based on parametric frequency conversion in an optical cavity, which has been widely investigated as a coherent light source with an extremely wide wavelength tuning range. However, steady oscillation in an OPO is confined by the cavity delay, which leads to difficulty in frequency tuning, and the frequency tuning is discrete with the minimum tuning step determined by the cavity delay. Here, we propose and demonstrate a counterpart of an OPO in the optoelectronic domain, i.e., an optoelectronic parametric oscillator (OEPO) based on parametric frequency conversion in an optoelectronic cavity to generate microwave signals. Owing to the unique energy-transition process in the optoelectronic cavity, the phase evolution in the OEPO is not linear, leading to steady single-mode oscillation or multimode oscillation that is not bounded by the cavity delay. Furthermore, the multimode oscillation in the OEPO is stable and easy to realize owing to the phase control of the parametric frequency-conversion process in the optoelectronic cavity, while stable multimode oscillation is difficult to achieve in conventional oscillators such as an optoelectronic oscillator (OEO) or an OPO due to the mode-hopping and mode-competition effect. The proposed OEPO has great potential in applications such as microwave signal generation, oscillator-based computation, and radio-frequency phase-stable transfer. Nature Publishing Group UK 2020-06-15 /pmc/articles/PMC7295800/ /pubmed/32566172 http://dx.doi.org/10.1038/s41377-020-0337-5 Text en © The Author(s) 2020 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/. |
spellingShingle | Article Hao, Tengfei Cen, Qizhuang Guan, Shanhong Li, Wei Dai, Yitang Zhu, Ninghua Li, Ming Optoelectronic parametric oscillator |
title | Optoelectronic parametric oscillator |
title_full | Optoelectronic parametric oscillator |
title_fullStr | Optoelectronic parametric oscillator |
title_full_unstemmed | Optoelectronic parametric oscillator |
title_short | Optoelectronic parametric oscillator |
title_sort | optoelectronic parametric oscillator |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7295800/ https://www.ncbi.nlm.nih.gov/pubmed/32566172 http://dx.doi.org/10.1038/s41377-020-0337-5 |
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