{"title":"Highly Efficient Acousto-Optic Modulation Driven by Ultra-Low Power in Integrated Photonic–Phononic Waveguides","authors":"Liang Zhang, Yongzhou Xue, Zewei Chen, Yanan Guo, Junxi Wang, Jinmin Li, Jianchang Yan","doi":"10.1002/lpor.202401952","DOIUrl":null,"url":null,"abstract":"Acousto-optic modulation (AOM) can tailor acoustic and optical domains, promising applications from signal processing to quantum transduction. Advances in integrated circuits technologies have facilitated minimization and integration of acousto-optic devices, paving ways for their applications in large-scale hybrid integrated photonic-phononic systems. Recently, integrated AOM is demonstrated with promising performance on various integrated piezoelectric materials. However, their optical conversion efficiencies remain significantly below unity. Achieving high efficiency necessitates strong mode-coupling over long interaction space, which requires strong confinement and minimizing losses for both acoustic and optical fields in integrated structures. This is challenging for most integrated material platforms. In this work, efficient AOM is demonstrated using semi-insulating gallium nitride (GaN) on sapphire. By leveraging the sub-wavelength confinement of both optical and acoustic fields within GaN waveguides, while minimizing optical (0.35 dB <span data-altimg=\"/cms/asset/ecb7abb6-9211-4441-bdd2-9810defb0b34/lpor202401952-math-0001.png\"></span><mjx-container ctxtmenu_counter=\"3\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" location=\"graphic/lpor202401952-math-0001.png\"><mjx-semantics><mjx-msup data-semantic-children=\"0,3\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"c m Superscript negative 1\" data-semantic-type=\"superscript\"><mjx-mi data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"4\" data-semantic-role=\"unknown\" data-semantic-type=\"identifier\"><mjx-c></mjx-c><mjx-c></mjx-c></mjx-mi><mjx-script style=\"vertical-align: 0.363em;\"><mjx-mrow data-semantic-annotation=\"clearspeak:simple\" data-semantic-children=\"2\" data-semantic-content=\"1\" data-semantic- data-semantic-parent=\"4\" data-semantic-role=\"negative\" data-semantic-type=\"prefixop\" size=\"s\"><mjx-mo data-semantic- data-semantic-operator=\"prefixop,−\" data-semantic-parent=\"3\" data-semantic-role=\"subtraction\" data-semantic-type=\"operator\" rspace=\"1\"><mjx-c></mjx-c></mjx-mo><mjx-mn data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"3\" data-semantic-role=\"integer\" data-semantic-type=\"number\"><mjx-c></mjx-c></mjx-mn></mjx-mrow></mjx-script></mjx-msup></mjx-semantics></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math altimg=\"urn:x-wiley:18638880:media:lpor202401952:lpor202401952-math-0001\" display=\"inline\" location=\"graphic/lpor202401952-math-0001.png\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><semantics><msup data-semantic-=\"\" data-semantic-children=\"0,3\" data-semantic-role=\"unknown\" data-semantic-speech=\"c m Superscript negative 1\" data-semantic-type=\"superscript\"><mi data-semantic-=\"\" data-semantic-font=\"normal\" data-semantic-parent=\"4\" data-semantic-role=\"unknown\" data-semantic-type=\"identifier\">cm</mi><mrow data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-children=\"2\" data-semantic-content=\"1\" data-semantic-parent=\"4\" data-semantic-role=\"negative\" data-semantic-type=\"prefixop\"><mo data-semantic-=\"\" data-semantic-operator=\"prefixop,−\" data-semantic-parent=\"3\" data-semantic-role=\"subtraction\" data-semantic-type=\"operator\">−</mo><mn data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"normal\" data-semantic-parent=\"3\" data-semantic-role=\"integer\" data-semantic-type=\"number\">1</mn></mrow></msup>${\\rm cm}^{-1}$</annotation></semantics></math></mjx-assistive-mml></mjx-container>) and acoustic (0.4 dB <span data-altimg=\"/cms/asset/5952d4a2-b120-4241-8ca4-a060ca090136/lpor202401952-math-0002.png\"></span><mjx-container ctxtmenu_counter=\"4\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" location=\"graphic/lpor202401952-math-0002.png\"><mjx-semantics><mjx-msup data-semantic-children=\"0,3\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"m m Superscript negative 1\" data-semantic-type=\"superscript\"><mjx-mi data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"4\" data-semantic-role=\"unknown\" data-semantic-type=\"identifier\"><mjx-c></mjx-c><mjx-c></mjx-c></mjx-mi><mjx-script style=\"vertical-align: 0.363em;\"><mjx-mrow data-semantic-annotation=\"clearspeak:simple\" data-semantic-children=\"2\" data-semantic-content=\"1\" data-semantic- data-semantic-parent=\"4\" data-semantic-role=\"negative\" data-semantic-type=\"prefixop\" size=\"s\"><mjx-mo data-semantic- data-semantic-operator=\"prefixop,−\" data-semantic-parent=\"3\" data-semantic-role=\"subtraction\" data-semantic-type=\"operator\" rspace=\"1\"><mjx-c></mjx-c></mjx-mo><mjx-mn data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"3\" data-semantic-role=\"integer\" data-semantic-type=\"number\"><mjx-c></mjx-c></mjx-mn></mjx-mrow></mjx-script></mjx-msup></mjx-semantics></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math altimg=\"urn:x-wiley:18638880:media:lpor202401952:lpor202401952-math-0002\" display=\"inline\" location=\"graphic/lpor202401952-math-0002.png\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><semantics><msup data-semantic-=\"\" data-semantic-children=\"0,3\" data-semantic-role=\"unknown\" data-semantic-speech=\"m m Superscript negative 1\" data-semantic-type=\"superscript\"><mi data-semantic-=\"\" data-semantic-font=\"normal\" data-semantic-parent=\"4\" data-semantic-role=\"unknown\" data-semantic-type=\"identifier\">mm</mi><mrow data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-children=\"2\" data-semantic-content=\"1\" data-semantic-parent=\"4\" data-semantic-role=\"negative\" data-semantic-type=\"prefixop\"><mo data-semantic-=\"\" data-semantic-operator=\"prefixop,−\" data-semantic-parent=\"3\" data-semantic-role=\"subtraction\" data-semantic-type=\"operator\">−</mo><mn data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"normal\" data-semantic-parent=\"3\" data-semantic-role=\"integer\" data-semantic-type=\"number\">1</mn></mrow></msup>${\\rm mm}^{-1}$</annotation></semantics></math></mjx-assistive-mml></mjx-container>) propagation losses, complete optical mode conversion of AOM driven by a 1.67-mW radio frequency power, setting a benchmark for integrated acousto-optical modulators, is achieved. Furthermore, the AOM non-reciprocity is also performed with high non-reciprocal contrast (<span data-altimg=\"/cms/asset/d6e6219c-a102-45db-b9a7-4591761d2d56/lpor202401952-math-0003.png\"></span><mjx-container ctxtmenu_counter=\"5\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" location=\"graphic/lpor202401952-math-0003.png\"><mjx-semantics><mjx-mo data-semantic- data-semantic-role=\"inequality\" data-semantic-speech=\"greater than\" data-semantic-type=\"relation\"><mjx-c></mjx-c></mjx-mo></mjx-semantics></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math altimg=\"urn:x-wiley:18638880:media:lpor202401952:lpor202401952-math-0003\" display=\"inline\" location=\"graphic/lpor202401952-math-0003.png\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><semantics><mo data-semantic-=\"\" data-semantic-role=\"inequality\" data-semantic-speech=\"greater than\" data-semantic-type=\"relation\">></mo>$>$</annotation></semantics></math></mjx-assistive-mml></mjx-container>10 dB) across a 4-GHz optical bandwidth. The work offers a robust and efficient acousto-optic platform, opening new opportunities for integrated quantum transduction, signal processing, and non-magnetic optical isolation.","PeriodicalId":204,"journal":{"name":"Laser & Photonics Reviews","volume":"18 1","pages":""},"PeriodicalIF":9.8000,"publicationDate":"2025-01-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Laser & Photonics Reviews","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1002/lpor.202401952","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"OPTICS","Score":null,"Total":0}
引用次数: 0
Abstract
Acousto-optic modulation (AOM) can tailor acoustic and optical domains, promising applications from signal processing to quantum transduction. Advances in integrated circuits technologies have facilitated minimization and integration of acousto-optic devices, paving ways for their applications in large-scale hybrid integrated photonic-phononic systems. Recently, integrated AOM is demonstrated with promising performance on various integrated piezoelectric materials. However, their optical conversion efficiencies remain significantly below unity. Achieving high efficiency necessitates strong mode-coupling over long interaction space, which requires strong confinement and minimizing losses for both acoustic and optical fields in integrated structures. This is challenging for most integrated material platforms. In this work, efficient AOM is demonstrated using semi-insulating gallium nitride (GaN) on sapphire. By leveraging the sub-wavelength confinement of both optical and acoustic fields within GaN waveguides, while minimizing optical (0.35 dB ) and acoustic (0.4 dB ) propagation losses, complete optical mode conversion of AOM driven by a 1.67-mW radio frequency power, setting a benchmark for integrated acousto-optical modulators, is achieved. Furthermore, the AOM non-reciprocity is also performed with high non-reciprocal contrast (10 dB) across a 4-GHz optical bandwidth. The work offers a robust and efficient acousto-optic platform, opening new opportunities for integrated quantum transduction, signal processing, and non-magnetic optical isolation.
期刊介绍:
Laser & Photonics Reviews is a reputable journal that publishes high-quality Reviews, original Research Articles, and Perspectives in the field of photonics and optics. It covers both theoretical and experimental aspects, including recent groundbreaking research, specific advancements, and innovative applications.
As evidence of its impact and recognition, Laser & Photonics Reviews boasts a remarkable 2022 Impact Factor of 11.0, according to the Journal Citation Reports from Clarivate Analytics (2023). Moreover, it holds impressive rankings in the InCites Journal Citation Reports: in 2021, it was ranked 6th out of 101 in the field of Optics, 15th out of 161 in Applied Physics, and 12th out of 69 in Condensed Matter Physics.
The journal uses the ISSN numbers 1863-8880 for print and 1863-8899 for online publications.