Author Affiliations
Abstract
1 Nankai University, TEDA Institute of Applied Physics, School of Physics, The MOE Key Laboratory of Weak-Light Nonlinear Photonics, Tianjin, China
2 Shanxi University, Collaborative Innovation Center of Extreme Optics, Taiyuan, China
3 INRS-EMT, Varennes, Quebec, Canada
4 University of Zagreb, Department of Physics, Faculty of Science, Zagreb, Croatia
Synthetic dimensions (SDs) opened the door for exploring previously inaccessible phenomena in high-dimensional space. However, construction of synthetic lattices with desired coupling properties is a challenging and unintuitive task. Here, we use deep learning artificial neural networks (ANNs) to construct lattices in real space with a predesigned spectrum of mode eigenvalues, and thus to validly design the dynamics in synthetic mode dimensions. By employing judiciously chosen perturbations (wiggling of waveguides at desired frequencies), we show resonant mode coupling and tailored dynamics in SDs. Two distinct examples are illustrated: one features uniform synthetic mode coupling, and the other showcases the edge defects that allow for tailored light transport and confinement. Furthermore, we demonstrate morphing of light into a topologically protected edge mode with modified Su–Schrieffer–Heeger photonic lattices. Such an ANN-assisted construction of SDs may advance toward “utopian networks,” opening new avenues for fundamental research beyond geometric limitations as well as for applications in mode lasing, optical switching, and communication technologies.
synthetic dimensions deep learning mode manipulation topological mode morphing photonic lattices 
Advanced Photonics
2024, 6(2): 026005
Author Affiliations
Abstract
1 Optical Sciences Centre, Swinburne University of Technology, Hawthorn, VIC 3122, Australia
2 Electro-Photonics Laboratory, Department of Electrical and Computer Systems Engineering, Monash University, VIC3800, Australia
3 School of Engineering, RMIT University, Melbourne, VIC 3001, Australia
4 Department of Physics, City University of Hong Kong, Hong Kong, China
5 State Key Laboratory of Transient Optics and Photonics, Xi'an Institute of Optics and Precision Mechanics, Chinese Academy of Science, Xi'an 710119, China
6 INRS -Énergie, Matériaux et Télécommunications, 1650 Boulevard Lionel-Boulet, Varennes, Québec, J3X 1S2, Canada
7 Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 610054, China
We review recent work on narrowband orthogonally polarized optical RF single sideband generators as well as dual-channel equalization, both based on high-Q integrated ring resonators. The devices operate in the optical telecommunications C-band and enable RF operation over a range of either fixed or thermally tuneable frequencies. They operate via TE/TM mode birefringence in the resonator. We achieve a very large dynamic tuning range of over 55 dB for both the optical carrier-to-sideband ratio and the dual-channel RF equalization for both the fixed and tunable devices.
Journal of Semiconductors
2021, 42(4): 041305
Author Affiliations
Abstract
1 Optical Sciences Centre, Swinburne University of Technology, Hawthorn, VIC 3122, Australia
2 Electro-Photonics Laboratory, Department of Electrical and Computer Systems Engineering, Monash University, VIC3800, Australia
3 School of Engineering, RMIT University, Melbourne, VIC 3001, Australia
4 Department of Physics, City University of Hong Kong, Hong Kong, China
5 State Key Laboratory of Transient Optics and Photonics, Xi'an Institute of Optics and Precision Mechanics, Chinese Academy of Science, Xi'an 710119, China
6 INRS -Énergie, Matériaux et Télécommunications, 1650 Boulevard Lionel-Boulet, Varennes, Québec, J3X 1S2, Canada
7 Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 610054, China
We review recent work on broadband RF channelizers based on integrated optical frequency Kerr micro-combs combined with passive micro-ring resonator filters, with microcombs having channel spacings of 200 and 49 GHz. This approach to realizing RF channelizers offers reduced complexity, size, and potential cost for a wide range of applications to microwave signal detection.
Journal of Semiconductors
2021, 42(4): 041302
Author Affiliations
Abstract
1 MOE Key Laboratory of Weak-Light Nonlinear Photonics, TEDA Applied Physics Institute and School of Physics, Nankai University, Tianjin 300457, China
2 INRS-EMT, 1650 Blvd. Lionel-Boulet, Varennes, Quebec J3X 1S2, Canada
3 Department of Applied Mathematics, University of Crete, Heraklion, Crete 71409, Greece
4 Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 610054, China
5 Institute of Applied and Computational Mathematics, FORTH, Heraklion, Crete 70013, Greece
6 Department of Physics & Astronomy, San Francisco State University, San Francisco, California 94132, USA
7 e-mail: morandotti@emt.inrs.ca
8 e-mail: zgchen@nankai.edu.cn
We demonstrate, both analytically and experimentally, free-space pin-like optical vortex beams (POVBs). Such angular-momentum-carrying beams feature tunable peak intensity and undergo robust antidiffracting propagation, realized by judiciously modulating both the amplitude and the phase profile of a standard laser beam. Specifically, they are generated by superimposing a radially symmetric power-law phase on a helical phase structure, which allows the inclusion of an orbital angular momentum term to the POVBs. During propagation in free space, these POVBs initially exhibit autofocusing dynamics, and subsequently their amplitude patterns morph into a high-order Bessel-like profile characterized by a hollow core and an annular main lobe with a constant or tunable width during propagation. In contrast with numerous previous endeavors on Bessel beams, our work represents the first demonstration of long-distance free-space generation of optical vortex “pins” with their peak intensity evolution controlled by the impressed amplitude structure. Both the Poynting vectors and the optical radiation forces associated with these beams are also numerically analyzed, revealing novel properties that may be useful for a wide range of applications.
Photonics Research
2021, 9(7): 07001204
Author Affiliations
Abstract
1 Institut National de la Recherche Scientifique (INRS), Centre Énergie, Matériaux et Télécommunications (EMT), Varennes, QC J3X 1S2, Canada
2 Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 610054, China
This paper is devoted to reviewing the results achieved so far in the application of the single-pixel imaging technique to terahertz (THz) systems. The use of THz radiation for imaging purposes has been largely explored in the last twenty years, due to the unique capabilities of this kind of radiation in interrogating material properties. However, THz imaging systems are still limited by the long acquisition time required to reconstruct the object image and significant efforts have been recently directed to overcome this drawback. One of the most promising approaches in this sense is the so-called "single-pixel" imaging, which in general enables image reconstruction by patterning the beam probing the object and measuring the total transmission (or reflection) with a single-pixel detector (i.e., with no spatial resolution). The main advantages of such technique are that i) no bulky moving parts are required to raster-scan the object and ii) compressed sensing (CS) algorithms, which allow an appropriate reconstruction of the image with an incomplete set of measurements, can be successfully implemented. Overall, this can result in a reduction of the acquisition time. In this review, we cover the experimental solutions proposed to implement such imaging technique at THz frequencies, as well as some practical uses for typical THz applications.
terahertz imaging single-pixel imaging compressed sensing 
Opto-Electronic Advances
2020, 3(9): 09200012
Author Affiliations
Abstract
1 Centre for Micro-Photonics, Swinburne University of Technology, Hawthorn, VIC 3122, Australia
2 ARC Centre of Excellence for Ultrahigh-bandwidth Devices for Optical Systems (CUDOS), RMIT University, Melbourne, VIC 3001, Australia
3 Department of Physics and Material Science, City University of Hong Kong, Tat Chee Avenue, Hong Kong, China
4 State Key Laboratory of Transient Optics and Photonics, Xi’an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Xi’an 710119, China
5 INRS-Énergie, Matériaux et Télécommunications, 1650 Boulevard Lionel-Boulet, Varennes, Québec J3X 1S2, Canada
6 National Research University of Information Technologies, Mechanics and Optics, St. Petersburg, Russia
7 Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 610054, China
We demonstrate significantly improved performance of a microwave true time delay line based on an integrated optical frequency comb source. The broadband micro-comb (over 100 nm wide) features a record low free spectral range (FSR) of 49 GHz, resulting in an unprecedented record high channel number (81 over the C band)—the highest number of channels for an integrated comb source used for microwave signal processing. We theoretically analyze the performance of a phased array antenna and show that this large channel count results in a high angular resolution and wide beam-steering tunable range. This demonstrates the feasibility of our approach as a competitive solution toward implementing integrated photonic true time delays in radar and communications systems.
Radio frequency photonics Nonlinear optics, integrated optics Phased-array radar 
Photonics Research
2018, 6(5): 05000B30
作者单位
摘要
1 Institut National de la Recherche Scientifique – Centre Energie, Materiaux et Telecommunications (INRS-EMT), 1650 Boulevard Lionel-Boulet, Varennes, Quebec, J3X 1S2, Canada
2 Department of Energy, Information Engineering and Mathematical Models, University of Palermo, Palermo, Italy
3 Department of Physics & Astronomy, University of Sussex, Falmer, Brighton BN1 9QH, UK
4 Department of Physics and Material Science, City University of Hong Kong, Tat Chee Avenue, Hong Kong, China
5 State Key Laboratory of Transient Optics and Photonics, Xi’an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Xi’an 710119, China
6 Centre for Micro Photonics, Swinburne University of Technology, Hawthorn, Victoria 3122, Australia
7 Institute of Photonics, Department of Physics, University of Strathclyde, Glasgow G1 1RD, UK
8 School of Engineering, University of Glasgow, Rankine Building, Oakfield Avenue, Glasgow G12 8LT, UK
9 Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 610054, China
10 National Research University of Information Technologies, Mechanics and Optics, St Petersburg 197101, Russia
nonlinear optics quantum optics entangled photons 
Frontiers of Optoelectronics
2018, 11(2): 134–147
Author Affiliations
Abstract
1 Emergent Photonics (Epic) Lab, Department of Physics and Astronomy, University of Sussex, Brighton BN1 9QH, UK
2 City University of Hong Kong, Tat Chee Avenue, Hong Kong, China
3 Centre for Microphotonics, Swinburne University of Technology, Hawthorn, VIC 3122, Australia
4 INRS-EMT, 1650 Boulevard Lionel-Boulet, Varennes, Québec J3X 1S2, Canada
5 Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 610054, China
6 National Research University of Information Technologies, Mechanics and Optics, St. Petersburg, Russia
7 Xi’an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Xi’an 710119, China
We experimentally demonstrate the generation of highly coherent Type-II micro-combs based on a micro-resonator nested in a fiber cavity loop, known as the filter-driven four wave mixing (FD-FWM) laser scheme. In this system, the frequency spacing of the comb can be adjusted to integer multiples of the free-spectral range (FSR) of the nested micro-resonator by properly tuning the fiber cavity length. Sub-comb lines with single FSR spacing around the primary comb lines can be generated. Such a spectral emission is known as a “Type-II comb”. Our system achieves a fully coherent output. This behavior is verified by numerical simulations. This study represents an important step forward in controlling and manipulating the dynamics of an FD-FWM laser.
Nonlinear optics, integrated optics Lasers, fiber Optical resonators 
Photonics Research
2018, 6(5): 05000B67

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