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Mobini E, Espinosa DHG, Vyas K, Dolgaleva K. AlGaAs Nonlinear Integrated Photonics. MICROMACHINES 2022; 13:mi13070991. [PMID: 35888808 PMCID: PMC9323658 DOI: 10.3390/mi13070991] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 04/09/2022] [Revised: 06/06/2022] [Accepted: 06/13/2022] [Indexed: 01/18/2023]
Abstract
Practical applications implementing integrated photonic circuits can benefit from nonlinear optical functionalities such as wavelength conversion, all-optical signal processing, and frequency-comb generation, among others. Numerous nonlinear waveguide platforms have been explored for these roles; the group of materials capable of combining both passive and active functionalities monolithically on the same chip is III–V semiconductors. AlGaAs is the most studied III–V nonlinear waveguide platform to date; it exhibits both second- and third-order optical nonlinearity and can be used for a wide range of integrated nonlinear photonic devices. In this review, we conduct an extensive overview of various AlGaAs nonlinear waveguide platforms and geometries, their nonlinear optical performances, as well as the measured values and wavelength dependencies of their effective nonlinear coefficients. Furthermore, we highlight the state-of-the-art achievements in the field, among which are efficient tunable wavelength converters, on-chip frequency-comb generation, and ultra-broadband on-chip supercontinuum generation. Moreover, we overview the applications in development where AlGaAs nonlinear functional devices aspire to be the game-changers. Among such applications, there is all-optical signal processing in optical communication networks and integrated quantum photonic circuits.
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Affiliation(s)
- Ehsan Mobini
- Department of Physics, University of Ottawa, Ottawa, ON K1N 6N5, Canada;
| | - Daniel H. G. Espinosa
- School of Electrical Engineering and Computer Science, University of Ottawa, Ottawa, ON K1N 6N5, Canada; (D.H.G.E.); (K.V.)
| | - Kaustubh Vyas
- School of Electrical Engineering and Computer Science, University of Ottawa, Ottawa, ON K1N 6N5, Canada; (D.H.G.E.); (K.V.)
| | - Ksenia Dolgaleva
- Department of Physics, University of Ottawa, Ottawa, ON K1N 6N5, Canada;
- School of Electrical Engineering and Computer Science, University of Ottawa, Ottawa, ON K1N 6N5, Canada; (D.H.G.E.); (K.V.)
- Correspondence:
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Yang Z, Zhang R, Wang Z, Xu P, Zhang W, Kang Z, Zheng J, Dai S, Wang R, Majumdar A. High-Q, submicron-confined chalcogenide microring resonators. OPTICS EXPRESS 2021; 29:33225-33233. [PMID: 34809138 DOI: 10.1364/oe.434808] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/24/2021] [Accepted: 09/23/2021] [Indexed: 06/13/2023]
Abstract
We demonstrate high quality (Q) factor microring resonators in high index-contrast GeSbSe chalcogenide glass waveguides using electron-beam lithography followed by plasma dry etching. A microring resonator with a radius of 90 μm shows an intrinsic Q factor of 4.1 × 105 in the telecom band. Thanks to the submicron waveguide dimension, the effective nonlinear coefficient was determined to be up to ∼110 W-1m-1 at 1550 nm, yielding a larger figure-of-merit compared with previously reported submicron chalcogenide waveguides. Such a high Q factor, combined with the large nonlinear coefficient and high confinement, shows the great potential of the GeSbSe microring resonator as a competitive platform in integrated nonlinear photonics.
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Liao Z, Wagner SJ, Alam MZ, Tolstikhin V, Stewart Aitchison J. Vertically integrated spot-size converter in AlGaAs-GaAs. OPTICS LETTERS 2017; 42:4167-4170. [PMID: 29028039 DOI: 10.1364/ol.42.004167] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/11/2017] [Accepted: 09/14/2017] [Indexed: 06/07/2023]
Abstract
We report on the demonstration of a spot size converter (SSC) for monolithic photonic integration at a wavelength of 850 nm on a GaAs substrate. We designed and fabricated a dual-waveguide AlGaAs chip. The design consists of a lower waveguide layer for efficient end-fire coupling to a single-mode fiber, an upper waveguide layer for high refractive index contrast waveguides, and a vertical SSC to connect the two waveguide layers. We measured a SSC conversion efficiency of 91% (or -0.4 dB) between the upper and lower waveguide layers for the TE mode at a wavelength of 850 nm.
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Saeidi S, Awan KM, Sirbu L, Dolgaleva K. Nonlinear photonics on-a-chip in III-V semiconductors: quest for promising material candidates. APPLIED OPTICS 2017; 56:5532-5541. [PMID: 29047512 DOI: 10.1364/ao.56.005532] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 02/23/2017] [Accepted: 06/06/2017] [Indexed: 06/07/2023]
Abstract
We propose several designs of nonlinear optical waveguides based on quaternary III-V semiconductors AlGaAsSb and InGaAsP. These semiconductor materials have been widely used for laser sources. Their nonlinear optical properties, however, yet remain unexplored, while the materials definitely hold promise for nonlinear photonics on-a-chip. The latter argument is based on the fact that III-V compounds tend to exhibit high values of the nonlinear optical susceptibilities, while the nonlinear absorption in these materials can be minimized in the wavelength range of interest through a proper selection of the material composition. We present the modal analysis for the designed waveguide structures and show that the effective mode area much less than 1 μm2 can be achieved through a design optimization in each of the two compounds. We also present specific waveguide designs that demonstrate zero dispersion at the wavelengths of interest. The designed AlGaAsSb and InGaAsP waveguides are thus expected to demonstrate high values of the nonlinear coefficient and efficient nonlinear optical interactions.
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Timofeeva M, Bouravleuv A, Cirlin G, Shtrom I, Soshnikov I, Reig Escalé M, Sergeyev A, Grange R. Polar Second-Harmonic Imaging to Resolve Pure and Mixed Crystal Phases along GaAs Nanowires. NANO LETTERS 2016; 16:6290-6297. [PMID: 27657488 DOI: 10.1021/acs.nanolett.6b02592] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/12/2023]
Abstract
In this work, we report an optical method for characterizing crystal phases along single-semiconductor III-V nanowires based on the measurement of polarization-dependent second-harmonic generation. This powerful imaging method is based on a per-pixel analysis of the second-harmonic-generated signal on the incoming excitation polarization. The dependence of the second-harmonic generation responses on the nonlinear second-order susceptibility tensor allows the distinguishing of areas of pure wurtzite, zinc blende, and mixed and rotational twins crystal structures in individual nanowires. With a far-field nonlinear optical microscope, we recorded the second-harmonic generation in GaAs nanowires and precisely determined their various crystal structures by analyzing the polar response for each pixel of the images. The predicted crystal phases in GaAs nanowire are confirmed with scanning transmission electron and high-resolution transmission electron measurements. The developed method of analyzing the nonlinear polar response of each pixel can be used for an investigation of nanowire crystal structure that is quick, sensitive to structural transitions, nondestructive, and on-the-spot. It can be applied for the crystal phase characterization of nanowires built into optoelectronic devices in which electron microscopy cannot be performed (for example, in lab-on-a-chip devices). Moreover, this method is not limited to GaAs nanowires but can be used for other nonlinear optical nanostructures.
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Affiliation(s)
- Maria Timofeeva
- Optical Nanomaterial Group, Institute for Quantum Electronics, Department of Physics, ETH Zurich , Auguste-Piccard Hof 1, 8093 Zurich, Switzerland
- ITMO University , Kronverkskiy 49, 197101 Saint Petersburg, Russia
| | - Alexei Bouravleuv
- St. Petersburg Academic University , Khlopina 8/3, 194021 Saint Petersburg, Russia
- Ioffe Institute , Politekhnicheskaya 29, 194021 Saint Petersburg, Russia
| | - George Cirlin
- St. Petersburg Academic University , Khlopina 8/3, 194021 Saint Petersburg, Russia
- ITMO University , Kronverkskiy 49, 197101 Saint Petersburg, Russia
- Ioffe Institute , Politekhnicheskaya 29, 194021 Saint Petersburg, Russia
| | - Igor Shtrom
- St. Petersburg Academic University , Khlopina 8/3, 194021 Saint Petersburg, Russia
- Ioffe Institute , Politekhnicheskaya 29, 194021 Saint Petersburg, Russia
| | - Ilya Soshnikov
- St. Petersburg Academic University , Khlopina 8/3, 194021 Saint Petersburg, Russia
- Ioffe Institute , Politekhnicheskaya 29, 194021 Saint Petersburg, Russia
| | - Marc Reig Escalé
- Optical Nanomaterial Group, Institute for Quantum Electronics, Department of Physics, ETH Zurich , Auguste-Piccard Hof 1, 8093 Zurich, Switzerland
| | - Anton Sergeyev
- Optical Nanomaterial Group, Institute for Quantum Electronics, Department of Physics, ETH Zurich , Auguste-Piccard Hof 1, 8093 Zurich, Switzerland
| | - Rachel Grange
- Optical Nanomaterial Group, Institute for Quantum Electronics, Department of Physics, ETH Zurich , Auguste-Piccard Hof 1, 8093 Zurich, Switzerland
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