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High-Q CMOS-integrated photonic crystal microcavity devices

Integrated optical resonators are necessary or beneficial in realizations of various functions in scaled photonic platforms, including filtering, modulation, and detection in classical communication systems, optical sensing, as well as addressing and control of solid state emitters for quantum techn...

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Autores principales: Mehta, Karan K., Orcutt, Jason S., Tehar-Zahav, Ofer, Sternberg, Zvi, Bafrali, Reha, Meade, Roy, Ram, Rajeev J.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2014
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3921634/
https://www.ncbi.nlm.nih.gov/pubmed/24518161
http://dx.doi.org/10.1038/srep04077
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author Mehta, Karan K.
Orcutt, Jason S.
Tehar-Zahav, Ofer
Sternberg, Zvi
Bafrali, Reha
Meade, Roy
Ram, Rajeev J.
author_facet Mehta, Karan K.
Orcutt, Jason S.
Tehar-Zahav, Ofer
Sternberg, Zvi
Bafrali, Reha
Meade, Roy
Ram, Rajeev J.
author_sort Mehta, Karan K.
collection PubMed
description Integrated optical resonators are necessary or beneficial in realizations of various functions in scaled photonic platforms, including filtering, modulation, and detection in classical communication systems, optical sensing, as well as addressing and control of solid state emitters for quantum technologies. Although photonic crystal (PhC) microresonators can be advantageous to the more commonly used microring devices due to the former's low mode volumes, fabrication of PhC cavities has typically relied on electron-beam lithography, which precludes integration with large-scale and reproducible CMOS fabrication. Here, we demonstrate wavelength-scale polycrystalline silicon (pSi) PhC microresonators with Qs up to 60,000 fabricated within a bulk CMOS process. Quasi-1D resonators in lateral p-i-n structures allow for resonant defect-state photodetection in all-silicon devices, exhibiting voltage-dependent quantum efficiencies in the range of a few 10 s of %, few-GHz bandwidths, and low dark currents, in devices with loaded Qs in the range of 4,300–9,300; one device, for example, exhibited a loaded Q of 4,300, 25% quantum efficiency (corresponding to a responsivity of 0.31 A/W), 3 GHz bandwidth, and 30 nA dark current at a reverse bias of 30 V. This work demonstrates the possibility for practical integration of PhC microresonators with active electro-optic capability into large-scale silicon photonic systems.
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spelling pubmed-39216342014-02-25 High-Q CMOS-integrated photonic crystal microcavity devices Mehta, Karan K. Orcutt, Jason S. Tehar-Zahav, Ofer Sternberg, Zvi Bafrali, Reha Meade, Roy Ram, Rajeev J. Sci Rep Article Integrated optical resonators are necessary or beneficial in realizations of various functions in scaled photonic platforms, including filtering, modulation, and detection in classical communication systems, optical sensing, as well as addressing and control of solid state emitters for quantum technologies. Although photonic crystal (PhC) microresonators can be advantageous to the more commonly used microring devices due to the former's low mode volumes, fabrication of PhC cavities has typically relied on electron-beam lithography, which precludes integration with large-scale and reproducible CMOS fabrication. Here, we demonstrate wavelength-scale polycrystalline silicon (pSi) PhC microresonators with Qs up to 60,000 fabricated within a bulk CMOS process. Quasi-1D resonators in lateral p-i-n structures allow for resonant defect-state photodetection in all-silicon devices, exhibiting voltage-dependent quantum efficiencies in the range of a few 10 s of %, few-GHz bandwidths, and low dark currents, in devices with loaded Qs in the range of 4,300–9,300; one device, for example, exhibited a loaded Q of 4,300, 25% quantum efficiency (corresponding to a responsivity of 0.31 A/W), 3 GHz bandwidth, and 30 nA dark current at a reverse bias of 30 V. This work demonstrates the possibility for practical integration of PhC microresonators with active electro-optic capability into large-scale silicon photonic systems. Nature Publishing Group 2014-02-12 /pmc/articles/PMC3921634/ /pubmed/24518161 http://dx.doi.org/10.1038/srep04077 Text en Copyright © 2014, Macmillan Publishers Limited. All rights reserved http://creativecommons.org/licenses/by-nc-sa/3.0/ This work is licensed under a Creative Commons Attribution-NonCommercial-ShareAlike 3.0 Unported License. To view a copy of this license, visit http://creativecommons.org/licenses/by-nc-sa/3.0/
spellingShingle Article
Mehta, Karan K.
Orcutt, Jason S.
Tehar-Zahav, Ofer
Sternberg, Zvi
Bafrali, Reha
Meade, Roy
Ram, Rajeev J.
High-Q CMOS-integrated photonic crystal microcavity devices
title High-Q CMOS-integrated photonic crystal microcavity devices
title_full High-Q CMOS-integrated photonic crystal microcavity devices
title_fullStr High-Q CMOS-integrated photonic crystal microcavity devices
title_full_unstemmed High-Q CMOS-integrated photonic crystal microcavity devices
title_short High-Q CMOS-integrated photonic crystal microcavity devices
title_sort high-q cmos-integrated photonic crystal microcavity devices
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3921634/
https://www.ncbi.nlm.nih.gov/pubmed/24518161
http://dx.doi.org/10.1038/srep04077
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