1
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Wang YT, Ye QH, Yan JY, Qiao Y, Liu YX, Ye YZ, Chen C, Cheng XT, Li CH, Zhang ZJ, Huang CN, Meng Y, Zou K, Zhan WK, Zhao C, Hu X, Tee CATH, Sha WEI, Huang Z, Liu H, Jin CY, Ying L, Liu F. Moiré cavity quantum electrodynamics. SCIENCE ADVANCES 2025; 11:eadv8115. [PMID: 40397724 DOI: 10.1126/sciadv.adv8115] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 01/08/2025] [Accepted: 04/14/2025] [Indexed: 05/23/2025]
Abstract
Quantum emitters are a key component in photonic quantum technologies. Enhancing single-photon emission by engineering their photonic environment is essential for improving overall efficiency in quantum information processing. However, this enhancement is often limited by the need for ultraprecise emitter placement within conventional photonic cavities. Inspired by the fascinating physics of moiré pattern, we propose a multilayer moiré photonic crystal with a robust isolated flatband. Theoretical analysis reveals that, with nearly infinite photonic density of states, the moiré cavity simultaneously has a high Purcell factor and large tolerance over the emitter's position, breaking the constraints of conventional cavities. We then experimentally demonstrate various cavity quantum electrodynamic phenomena with a quantum dot in moiré cavity. A large tuning range (up to 40-fold) of quantum dot's radiative lifetime is achieved through strong Purcell enhancement and inhibition effects. Our findings open the door for moiré flatband cavity-enhanced quantum light sources and quantum nodes for the quantum internet.
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Affiliation(s)
- Yu-Tong Wang
- State Key Laboratory of Extreme Photonics and Instrumentation, College of Information Science and Electronic Engineering, Zhejiang University, Hangzhou 310027, China
| | - Qi-Hang Ye
- School of Physics, Zhejiang Key Laboratory of Micro-nano Quantum Chips and Quantum Control, Zhejiang University, Hangzhou 310027, China
| | - Jun-Yong Yan
- State Key Laboratory of Extreme Photonics and Instrumentation, College of Information Science and Electronic Engineering, Zhejiang University, Hangzhou 310027, China
| | - Yufei Qiao
- State Key Laboratory of Extreme Photonics and Instrumentation, College of Information Science and Electronic Engineering, Zhejiang University, Hangzhou 310027, China
- School of Physics, Zhejiang Key Laboratory of Micro-nano Quantum Chips and Quantum Control, Zhejiang University, Hangzhou 310027, China
| | - Yu-Xin Liu
- School of Physics, Zhejiang Key Laboratory of Micro-nano Quantum Chips and Quantum Control, Zhejiang University, Hangzhou 310027, China
| | - Yong-Zheng Ye
- State Key Laboratory of Extreme Photonics and Instrumentation, College of Information Science and Electronic Engineering, Zhejiang University, Hangzhou 310027, China
- International Joint Innovation Center, Zhejiang University, Haining 314400, China
| | - Chen Chen
- State Key Laboratory of Extreme Photonics and Instrumentation, College of Information Science and Electronic Engineering, Zhejiang University, Hangzhou 310027, China
| | - Xiao-Tian Cheng
- State Key Laboratory of Extreme Photonics and Instrumentation, College of Information Science and Electronic Engineering, Zhejiang University, Hangzhou 310027, China
| | - Chen-Hui Li
- State Key Laboratory of Extreme Photonics and Instrumentation, College of Information Science and Electronic Engineering, Zhejiang University, Hangzhou 310027, China
| | - Zi-Jian Zhang
- State Key Laboratory of Extreme Photonics and Instrumentation, College of Information Science and Electronic Engineering, Zhejiang University, Hangzhou 310027, China
| | - Cheng-Nian Huang
- State Key Laboratory of Extreme Photonics and Instrumentation, College of Information Science and Electronic Engineering, Zhejiang University, Hangzhou 310027, China
| | - Yun Meng
- School of Precision Instrument and Optoelectronic Engineering, Tianjin University, Tianjin 300072, China
- Key Laboratory of Optoelectronic Information Science and Technology, Ministry of Education, Tianjin 300072, China
| | - Kai Zou
- School of Precision Instrument and Optoelectronic Engineering, Tianjin University, Tianjin 300072, China
- Key Laboratory of Optoelectronic Information Science and Technology, Ministry of Education, Tianjin 300072, China
| | - Wen-Kang Zhan
- Laboratory of Solid State Optoelectronics Information Technology, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
- College of Materials Science and Opto-Electronic Technology, University of Chinese Academy of Science, Beijing 101804, China
| | - Chao Zhao
- Laboratory of Solid State Optoelectronics Information Technology, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
- College of Materials Science and Opto-Electronic Technology, University of Chinese Academy of Science, Beijing 101804, China
| | - Xiaolong Hu
- School of Precision Instrument and Optoelectronic Engineering, Tianjin University, Tianjin 300072, China
- Key Laboratory of Optoelectronic Information Science and Technology, Ministry of Education, Tianjin 300072, China
| | - Clarence Augustine T H Tee
- College of Physics and Electrical Information Engineering, Zhejiang Normal University, Hangzhou 310058, China
| | - Wei E I Sha
- State Key Laboratory of Extreme Photonics and Instrumentation, College of Information Science and Electronic Engineering, Zhejiang University, Hangzhou 310027, China
| | - Zhixiang Huang
- Key Laboratory of Intelligent Computing and Signal Processing, Ministry of Education, Anhui University, Hefei 230039, China
| | - Huiyun Liu
- Department of Electronic and Electrical Engineering, University College London, London WC1E 7JE, UK
| | - Chao-Yuan Jin
- State Key Laboratory of Extreme Photonics and Instrumentation, College of Information Science and Electronic Engineering, Zhejiang University, Hangzhou 310027, China
- International Joint Innovation Center, Zhejiang University, Haining 314400, China
- ZJU-Hangzhou Global Scientific and Technological Innovation Center, Zhejiang University, Hangzhou, Zhejiang 311200, China
| | - Lei Ying
- School of Physics, Zhejiang Key Laboratory of Micro-nano Quantum Chips and Quantum Control, Zhejiang University, Hangzhou 310027, China
| | - Feng Liu
- State Key Laboratory of Extreme Photonics and Instrumentation, College of Information Science and Electronic Engineering, Zhejiang University, Hangzhou 310027, China
- International Joint Innovation Center, Zhejiang University, Haining 314400, China
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2
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Kim K, Park K, Park H, Yu S, Park N, Piao X. Programmable photonic unitary circuits for light computing. NANOPHOTONICS (BERLIN, GERMANY) 2025; 14:1429-1449. [PMID: 40444196 PMCID: PMC12116228 DOI: 10.1515/nanoph-2024-0602] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 11/03/2024] [Accepted: 12/19/2024] [Indexed: 06/02/2025]
Abstract
Unitarity serves as a fundamental concept for characterizing linear and conservative wave phenomena in both classical and quantum systems. Developing platforms that perform unitary operations on light waves in a universal and programmable manner enables the emulation of complex light-matter interactions and the execution of general-purpose functionalities for wave manipulations, photonic computing, and quantum circuits. Recently, numerous approaches to implementing programmable photonic unitary circuits have been proposed and demonstrated, each employing different design strategies that distinctly impact overall device performance. Here, we review foundational design principles and recent achievements in the implementation of programmable photonic unitary circuits, with a particular focus on integrated photonic platforms. We classify the design strategies based on the dimensionality of nontrivial unit operations in their building blocks: lower-dimensional unitary units, such as SU(2) operations, and higher-dimensional ones, such as Fourier transforms. In each category, recent efforts to leverage alternative physical axes, such as the temporal and frequency domains, to address scalability challenges are also reviewed. We discuss the underlying concepts, design procedures, and trade-offs of each design strategy, especially in relation to light-based computing.
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Affiliation(s)
- Kyuho Kim
- Intelligent Wave Systems Laboratory, Department of Electrical and Computer Engineering, Seoul National University, Seoul08826, Korea
| | - Kunwoo Park
- Intelligent Wave Systems Laboratory, Department of Electrical and Computer Engineering, Seoul National University, Seoul08826, Korea
| | - Hyungchul Park
- Intelligent Wave Systems Laboratory, Department of Electrical and Computer Engineering, Seoul National University, Seoul08826, Korea
| | - Sunkyu Yu
- Intelligent Wave Systems Laboratory, Department of Electrical and Computer Engineering, Seoul National University, Seoul08826, Korea
| | - Namkyoo Park
- Photonic Systems Laboratory, Department of Electrical and Computer Engineering, Seoul National University, Seoul08826, Korea
| | - Xianji Piao
- Wave Engineering Laboratory, School of Electrical and Computer Engineering, University of Seoul, Seoul02504, Korea
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3
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Ye R, Li G, Wan S, Xue X, Wang PY, Qiao X, Wang L, Li H, Liu S, Wang J, Ma R, Bo F, Zheng Y, Dong CH, Yuan L, Chen X. Construction of Various Time-Varying Hamiltonians on Thin-Film Lithium Niobate Chip. PHYSICAL REVIEW LETTERS 2025; 134:163802. [PMID: 40344099 DOI: 10.1103/physrevlett.134.163802] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/06/2024] [Revised: 03/18/2025] [Accepted: 03/24/2025] [Indexed: 05/11/2025]
Abstract
Integrated photonics provides an important platform for simulating physical models with high-performance chip-scale devices, where the lattice size and the time dependence of a model are key ingredients for further enriching the functionality of a photonic chip. Here, we propose and demonstrate the construction of various time-varying Hamiltonian models using a single microresonator on thin-film lithium niobate chip. Such an integrated microresonator holds high-quality factor to 10^{6}, and supports the construction of the synthetic frequency lattice with effective lattice sites up to 221 under efficient integrated electro-optic modulation. By further applying different bichromatic modulations composed of two radio-frequency signals oppositely detuned from the resonant frequency in the microresonator, we successfully build various time-varying Hamiltonian models, where the temporal features of the dynamic band structures are captured from experimental measurements, highlighting great flexibility and tunability of this integrated chip. Our work presents a photonic chip for simulating versatile time-varying Hamiltonians, which pushes forward quantum simulations and future photonic applications.
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Affiliation(s)
- Rui Ye
- Shanghai Jiao Tong University, State Key Laboratory of Photonics and Communications, School of Physics and Astronomy, Shanghai 200240, China
| | - Guangzhen Li
- Shanghai Jiao Tong University, State Key Laboratory of Photonics and Communications, School of Physics and Astronomy, Shanghai 200240, China
| | - Shuai Wan
- University of Science and Technology of China, CAS Key Laboratory of Quantum Information, Hefei, Anhui 230026, China
- University of Science and Technology of China, CAS Center for Excellence in Quantum Information and Quantum Physics, Hefei, Anhui 230088, China
| | - Xiaotian Xue
- Shanghai Jiao Tong University, State Key Laboratory of Photonics and Communications, School of Physics and Astronomy, Shanghai 200240, China
| | - Pi-Yu Wang
- University of Science and Technology of China, CAS Key Laboratory of Quantum Information, Hefei, Anhui 230026, China
- University of Science and Technology of China, CAS Center for Excellence in Quantum Information and Quantum Physics, Hefei, Anhui 230088, China
| | - Xin Qiao
- Northwest Normal University, College of Physics and Electronics Engineering, Lanzhou 730070, China
| | - Luojia Wang
- Shanghai Jiao Tong University, State Key Laboratory of Photonics and Communications, School of Physics and Astronomy, Shanghai 200240, China
| | - Hao Li
- Shanghai Jiao Tong University, State Key Laboratory of Photonics and Communications, School of Physics and Astronomy, Shanghai 200240, China
| | - Shijie Liu
- Shanghai Jiao Tong University, State Key Laboratory of Photonics and Communications, School of Physics and Astronomy, Shanghai 200240, China
| | - Jiayu Wang
- Shanghai Jiao Tong University, State Key Laboratory of Photonics and Communications, School of Physics and Astronomy, Shanghai 200240, China
| | - Rui Ma
- Nankai University, MOE Key Laboratory of Weak-Light Nonlinear Photonics, TEDA Applied Physics Institute and School of Physics, Tianjin 300457, China
| | - Fang Bo
- Nankai University, MOE Key Laboratory of Weak-Light Nonlinear Photonics, TEDA Applied Physics Institute and School of Physics, Tianjin 300457, China
| | - Yuanlin Zheng
- Shanghai Jiao Tong University, State Key Laboratory of Photonics and Communications, School of Physics and Astronomy, Shanghai 200240, China
- Shanghai Research Center for Quantum Sciences, Shanghai 201315 China
| | - Chun-Hua Dong
- University of Science and Technology of China, CAS Key Laboratory of Quantum Information, Hefei, Anhui 230026, China
- University of Science and Technology of China, CAS Center for Excellence in Quantum Information and Quantum Physics, Hefei, Anhui 230088, China
| | - Luqi Yuan
- Shanghai Jiao Tong University, State Key Laboratory of Photonics and Communications, School of Physics and Astronomy, Shanghai 200240, China
| | - Xianfeng Chen
- Shanghai Jiao Tong University, State Key Laboratory of Photonics and Communications, School of Physics and Astronomy, Shanghai 200240, China
- Shanghai Research Center for Quantum Sciences, Shanghai 201315 China
- Collaborative Innovation Center of Light Manipulations and Applications, Shandong Normal University, Jinan 250358, China
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4
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Wang Z, Li K, Wang Y, Zhou X, Cheng Y, Jing B, Sun F, Li J, Li Z, Wu B, Gong Q, He Q, Li BB, Yang QF. Large-scale cluster quantum microcombs. LIGHT, SCIENCE & APPLICATIONS 2025; 14:164. [PMID: 40240777 PMCID: PMC12003720 DOI: 10.1038/s41377-025-01812-2] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/23/2025] [Revised: 02/07/2025] [Accepted: 03/04/2025] [Indexed: 04/18/2025]
Abstract
An optical frequency comb comprises a cluster of equally spaced, phase-locked spectral lines. Replacing these classical components with correlated quantum light gives rise to cluster quantum frequency combs, providing abundant quantum resources for measurement-based quantum computation, and multi-user quantum networks. We propose and generate cluster quantum microcombs within an on-chip optical microresonator driven by multi-frequency lasers. Through resonantly enhanced four-wave mixing processes, continuous-variable cluster states with 60 qumodes are deterministically created. The graph structures can be programmed into one- and two-dimensional lattices by adjusting the configurations of the pump lines, which are confirmed inseparable based on the measured covariance matrices. Our work demonstrates the largest-scale cluster states with unprecedented raw squeezing levels from a photonic chip, offering a compact and scalable platform for computational and communicational tasks with quantum advantages.
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Affiliation(s)
- Ze Wang
- State Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, 100871, Beijing, China
| | - Kangkang Li
- State Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, 100871, Beijing, China.
| | - Yue Wang
- State Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, 100871, Beijing, China
| | - Xin Zhou
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, 100190, Beijing, China
| | - Yinke Cheng
- State Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, 100871, Beijing, China
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, 100190, Beijing, China
| | - Boxuan Jing
- State Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, 100871, Beijing, China
| | - Fengxiao Sun
- State Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, 100871, Beijing, China
| | - Jincheng Li
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, 100190, Beijing, China
| | - Zhilin Li
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, 100190, Beijing, China
| | - Bingyan Wu
- State Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, 100871, Beijing, China
| | - Qihuang Gong
- State Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, 100871, Beijing, China
- Collaborative Innovation Center of Extreme Optics, Shanxi University, 030006, Taiyuan, China
- Peking University Yangtze Delta Institute of Optoelectronics, 226010, Nantong, Jiangsu, China
- Hefei National Laboratory, 230088, Hefei, China
| | - Qiongyi He
- State Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, 100871, Beijing, China.
- Collaborative Innovation Center of Extreme Optics, Shanxi University, 030006, Taiyuan, China.
- Peking University Yangtze Delta Institute of Optoelectronics, 226010, Nantong, Jiangsu, China.
- Hefei National Laboratory, 230088, Hefei, China.
| | - Bei-Bei Li
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, 100190, Beijing, China.
| | - Qi-Fan Yang
- State Key Laboratory for Artificial Microstructure and Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, 100871, Beijing, China.
- Collaborative Innovation Center of Extreme Optics, Shanxi University, 030006, Taiyuan, China.
- Peking University Yangtze Delta Institute of Optoelectronics, 226010, Nantong, Jiangsu, China.
- Hefei National Laboratory, 230088, Hefei, China.
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5
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Huang J, Miranda A, Liu W, Cheng X, Dwir B, Rudra A, Chang KC, Kapon E, Wong CW. Spatial quantum-interference landscapes of multi-site-controlled quantum dots coupled to extended photonic cavity modes. COMMUNICATIONS PHYSICS 2025; 8:152. [PMID: 40224499 PMCID: PMC11991910 DOI: 10.1038/s42005-025-02051-y] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 07/16/2024] [Accepted: 03/18/2025] [Indexed: 04/15/2025]
Abstract
A compact platform to integrate emitters in a cavity-like support is to embed quantum dots (QDs) in a photonic crystal (PhC) structure, making them promising candidates for integrated quantum photonic circuits. The emission properties of QDs can be modified by tailored photonic structures, relying on the Purcell effect or strong light-matter interactions. However, the effects of photonic states on spatial features of exciton emissions in these systems are rarely explored. Such effect is difficult to access due to random positions of self-assembled QDs in PhC structures, and the fact that quantum well excitons' wavefunctions resemble photonic states in a conventional distributed Bragg reflector cavity system. In this work, we instead observe a spatial signature of exciton emission using site-controlled QDs embedded in PhC cavities. In particular, we observe the detuning-dependent spatial repulsion of the QD exciton emissions by polarized imaging of the micro-photoluminescence, dependent on the controlled QD's position in a spatially extended photonic pattern. The observed effect arises due to the quantum interference between QD decay channel in a spatially-extended cavity mode. Our findings suggest that integration of site-controlled QDs in tailored photonic structures can enable spatially distributed single-photon sources and photon switches.
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Affiliation(s)
- Jiahui Huang
- Mesoscopic Optics and Quantum Electronics Laboratory, Department of Electrical and Computer Engineering, University of California, 420 Westwood Plaza, Los Angeles, CA 90095 USA
- Present Address: Xi’an Institute of Optics and Precision Mechanics, Chinese Academy of Science (CAS), 710119 Xi’an, China
| | - Alessio Miranda
- Institute of Physics, École Polytechnique Fédérale de Lausanne, Lausanne, VD 1015 Switzerland
| | - Wei Liu
- Mesoscopic Optics and Quantum Electronics Laboratory, Department of Electrical and Computer Engineering, University of California, 420 Westwood Plaza, Los Angeles, CA 90095 USA
| | - Xiang Cheng
- Mesoscopic Optics and Quantum Electronics Laboratory, Department of Electrical and Computer Engineering, University of California, 420 Westwood Plaza, Los Angeles, CA 90095 USA
| | - Benjamin Dwir
- Institute of Physics, École Polytechnique Fédérale de Lausanne, Lausanne, VD 1015 Switzerland
| | - Alok Rudra
- Institute of Physics, École Polytechnique Fédérale de Lausanne, Lausanne, VD 1015 Switzerland
| | - Kai-Chi Chang
- Mesoscopic Optics and Quantum Electronics Laboratory, Department of Electrical and Computer Engineering, University of California, 420 Westwood Plaza, Los Angeles, CA 90095 USA
| | - Eli Kapon
- Institute of Physics, École Polytechnique Fédérale de Lausanne, Lausanne, VD 1015 Switzerland
| | - Chee Wei Wong
- Mesoscopic Optics and Quantum Electronics Laboratory, Department of Electrical and Computer Engineering, University of California, 420 Westwood Plaza, Los Angeles, CA 90095 USA
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6
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Zhu Y, Shang J, Fan YN, Kou Y, Qu X, Yan XA, Zhang Y, Wang F. Implementation of double Feynman gate in high dimensional quantum systems. Sci Rep 2025; 15:12184. [PMID: 40205007 PMCID: PMC11982281 DOI: 10.1038/s41598-025-97002-6] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 01/01/2025] [Accepted: 04/01/2025] [Indexed: 04/11/2025] Open
Abstract
The photonic platform has emerged as a preferred choice for quantum computing and information processing due to its low loss and high integration capabilities. In the present research, we propose a high-dimensional double Feynman gate utilizing single-photon hybrid degrees of freedom coding. This gate can manipulate two qubits simultaneously, demonstrating effective quantum state conversion. Our experimental design offers valuable insights for the investigation of high-dimensional optical quantum logic gates and advances quantum fundamental research.
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Affiliation(s)
- Yanbing Zhu
- School of Science, Xi'an Polytechnic University, Xi'an, 710048, Shaanxi, China
| | - Jiaqi Shang
- School of Science, Xi'an Polytechnic University, Xi'an, 710048, Shaanxi, China
| | - Ya-Nan Fan
- School of Science, Xi'an Polytechnic University, Xi'an, 710048, Shaanxi, China
| | - Yunjie Kou
- School of Science, Xi'an Polytechnic University, Xi'an, 710048, Shaanxi, China
| | - Xiaofei Qu
- School of Science, Xi'an Polytechnic University, Xi'an, 710048, Shaanxi, China
| | - Xiang-An Yan
- School of Science, Xi'an Polytechnic University, Xi'an, 710048, Shaanxi, China
| | - Yunjie Zhang
- School of Science, Xi'an Polytechnic University, Xi'an, 710048, Shaanxi, China
| | - Feiran Wang
- School of Science, Xi'an Polytechnic University, Xi'an, 710048, Shaanxi, China.
- Ministry of Education Key Laboratory for Non-Equilibrium Synthesis and Modulation of Condensed Matter, Shaanxi Key Laboratory of Quantum Information and Quantum Optoelectronic Devices, School of Physics of Xi'an Jiaotong University, Xi'an, 710049, Shaanxi, China.
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7
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Du Y, Li BH, Hua X, Cao XY, Zhao Z, Xie F, Zhang Z, Yin HL, Xiao X, Wei K. Chip-integrated quantum signature network over 200 km. LIGHT, SCIENCE & APPLICATIONS 2025; 14:108. [PMID: 40038238 DOI: 10.1038/s41377-025-01775-4] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/01/2024] [Revised: 01/24/2025] [Accepted: 01/31/2025] [Indexed: 03/06/2025]
Abstract
The development of quantum networks is paramount towards practical and secure communications. Quantum digital signatures (QDS) offer an information-theoretically secure solution for ensuring data integrity, authenticity, and non-repudiation, rapidly growing from proof-of-concept to robust demonstrations. However, previous QDS systems relied on expensive and bulky optical equipment, limiting large-scale deployment and reconfigurable networking construction. Here, we introduce and verify a chip-based QDS network, placing the complicated and expensive measurement devices in the central relay while each user needs only a low-cost transmitter. We demonstrate the network with a three-node setup using an integrated encoder chip and decoder chip. By developing a 1-decoy-state one-time universal hashing-QDS protocol, we achieve a maximum signature rate of 0.0414 times per second for a 1 Mbit messages over fiber distances up to 200 km, surpassing all current state-of-the-art QDS experiments. This study validates the feasibility of chip-based QDS, paving the way for large-scale deployment and integration with existing fiber infrastructure.
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Affiliation(s)
- Yongqiang Du
- Guangxi Key Laboratory for Relativistic Astrophysics, School of Physical Science and Technology, Guangxi University, Nanning, 530004, China
| | - Bing-Hong Li
- National Laboratory of Solid State Microstructures and School of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing, 210093, China
| | - Xin Hua
- National Information Optoelectronics Innovation Center (NOEIC), Wuhan, 430074, China
| | - Xiao-Yu Cao
- National Laboratory of Solid State Microstructures and School of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing, 210093, China
| | - Zhengeng Zhao
- Guangxi Key Laboratory for Relativistic Astrophysics, School of Physical Science and Technology, Guangxi University, Nanning, 530004, China
| | - Feng Xie
- Guangxi Key Laboratory for Relativistic Astrophysics, School of Physical Science and Technology, Guangxi University, Nanning, 530004, China
- Guangxi Key Laboratory of Multimedia Communications and Network Technology, School of Computer, Electronics, and Information, Guangxi University, Nanning, 530004, China
| | - Zhenrong Zhang
- Guangxi Key Laboratory of Multimedia Communications and Network Technology, School of Computer, Electronics, and Information, Guangxi University, Nanning, 530004, China
| | - Hua-Lei Yin
- National Laboratory of Solid State Microstructures and School of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing, 210093, China.
- Department of Physics and Beijing Key Laboratory of Opto-electronic Functional Materials and Micro-nano Devices, Key Laboratory of Quantum State Construction and Manipulation (Ministry of Education), Renmin University of China, Beijing, 100872, China.
| | - Xi Xiao
- National Information Optoelectronics Innovation Center (NOEIC), Wuhan, 430074, China.
- Peng Cheng Laboratory, Shenzhen, 518055, China.
| | - Kejin Wei
- Guangxi Key Laboratory for Relativistic Astrophysics, School of Physical Science and Technology, Guangxi University, Nanning, 530004, China.
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8
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Jia X, Zhai C, Zhu X, You C, Cao Y, Zhang X, Zheng Y, Fu Z, Mao J, Dai T, Chang L, Su X, Gong Q, Wang J. Continuous-variable multipartite entanglement in an integrated microcomb. Nature 2025; 639:329-336. [PMID: 39972136 PMCID: PMC11903341 DOI: 10.1038/s41586-025-08602-1] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 04/16/2024] [Accepted: 01/07/2025] [Indexed: 02/21/2025]
Abstract
The generation of large-scale entangled states is crucial for quantum technologies, such as quantum computation1, communication2 and metrology3. Integrated quantum photonics that enables on-chip encoding, processing and detection of quantum light states offers a promising platform for the generation and manipulation of large-scale entangled states4,5. Generating entanglement between qubits encoded in discrete variables within single photons is challenging, owing to the difficulty of making single photons interact on photonic chips6-11. Devices that operate with continuous variables are more promising, as they enable the deterministic generation and entanglement of qumodes, in which information is encoded in light quadratures. Demonstrations so far have been limited to entanglement between two qumodes12-20. Here we report the deterministic generation of a continuous-variable eight-mode entanglement on an integrated optical chip. The chip delivers a quantum microcomb that produces multimode squeezed-vacuum optical frequency combs below the threshold. We verify the inseparability of our eight-mode state and demonstrate supermode multipartite entanglement over hundreds of megahertz sideband frequencies through violation of the van Loock-Furusawa criteria. By measuring the full matrices of nullifier correlations with sufficiently low off-diagonal noises, we characterize multipartite entanglement structures, which are approximate to the expected cluster-type structures for finite squeezing. This work shows the potential of continuous-variable integrated photonic quantum devices for facilitating quantum computing, networking and sensing.
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Affiliation(s)
- Xinyu Jia
- State Key Laboratory for Mesoscopic Physics, School of Physics, Peking University, Beijing, China
- Beijing Academy of Quantum Information Sciences, Beijing, China
| | - Chonghao Zhai
- State Key Laboratory for Mesoscopic Physics, School of Physics, Peking University, Beijing, China
| | - Xuezhi Zhu
- State Key Laboratory of Quantum Optics Technologies and Devices, Institute of Opto-Electronics, Shanxi University, Taiyuan, China
| | - Chang You
- State Key Laboratory for Mesoscopic Physics, School of Physics, Peking University, Beijing, China
| | - Yunyun Cao
- State Key Laboratory of Quantum Optics Technologies and Devices, Institute of Opto-Electronics, Shanxi University, Taiyuan, China
| | - Xuguang Zhang
- State Key Laboratory of Advanced Optical Communications System and Networks, School of Electronics, Peking University, Beijing, China
| | - Yun Zheng
- State Key Laboratory for Mesoscopic Physics, School of Physics, Peking University, Beijing, China
| | - Zhaorong Fu
- State Key Laboratory for Mesoscopic Physics, School of Physics, Peking University, Beijing, China
| | - Jun Mao
- State Key Laboratory for Mesoscopic Physics, School of Physics, Peking University, Beijing, China
| | - Tianxiang Dai
- State Key Laboratory for Mesoscopic Physics, School of Physics, Peking University, Beijing, China
| | - Lin Chang
- State Key Laboratory of Advanced Optical Communications System and Networks, School of Electronics, Peking University, Beijing, China
| | - Xiaolong Su
- State Key Laboratory of Quantum Optics Technologies and Devices, Institute of Opto-Electronics, Shanxi University, Taiyuan, China.
- Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan, China.
| | - Qihuang Gong
- State Key Laboratory for Mesoscopic Physics, School of Physics, Peking University, Beijing, China
- Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan, China
- Frontiers Science Center for Nano-optoelectronics & Collaborative Innovation Center of Quantum Matter, Peking University, Beijing, China
- Peking University Yangtze Delta Institute of Optoelectronics, Nantong, China
- Hefei National Laboratory, Hefei, China
| | - Jianwei Wang
- State Key Laboratory for Mesoscopic Physics, School of Physics, Peking University, Beijing, China.
- Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan, China.
- Frontiers Science Center for Nano-optoelectronics & Collaborative Innovation Center of Quantum Matter, Peking University, Beijing, China.
- Peking University Yangtze Delta Institute of Optoelectronics, Nantong, China.
- Hefei National Laboratory, Hefei, China.
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9
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Lu Y, Liao Z, Wang XH. Atomic-Scale On-Demand Photon Polarization Manipulation with High Efficiency for Integrated Photonic Chips. PHYSICAL REVIEW LETTERS 2025; 134:083601. [PMID: 40085857 DOI: 10.1103/physrevlett.134.083601] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/06/2023] [Revised: 01/08/2025] [Accepted: 02/03/2025] [Indexed: 03/16/2025]
Abstract
In order to overcome the challenge of lacking polarization encoding in integrated quantum photonic circuits, we propose a scheme to realize arbitrary polarization manipulation of a single photon by integrating a single quantum emitter in a photonic waveguide. In our scheme, one transition path of the three-level emitter is designed to simultaneously couple with two orthogonal polarization degenerate modes in the waveguide with adjustable coupling strengths, and the other transition path of the three-level emitter is driven by an external coherent field. The proposed polarization converter has several advantages, including arbitrary polarization conversion for any input polarization, tunable working frequency, excellent antidissipation ability with high-conversion efficiency, and atomic-scale size. Our Letter provides an effective solution to enable the polarization encoding of photons that can be applied in the integrated quantum photonic circuits, and will boost quantum photonic chips.
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Affiliation(s)
- Yunning Lu
- Sun Yat-sen University, State Key Laboratory of Optoelectronic Materials and Technologies, School of Physics, Guangzhou 510275, China
- Anhui University of Technology, School of Electrical and Information Engineering, Ma'anshan, 243002, China
| | - Zeyang Liao
- Sun Yat-sen University, State Key Laboratory of Optoelectronic Materials and Technologies, School of Physics, Guangzhou 510275, China
| | - Xue-Hua Wang
- Sun Yat-sen University, State Key Laboratory of Optoelectronic Materials and Technologies, School of Physics, Guangzhou 510275, China
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10
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Shultz N, McLeod E. Building blocks for nanophotonic devices and metamaterials. Chem Commun (Camb) 2025; 61:3301-3318. [PMID: 39876674 DOI: 10.1039/d4cc06236a] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/30/2025]
Abstract
Nanophotonic devices control and manipulate light at the nanometer scale. Applications include biological imaging, integrated photonic circuits, and metamaterials. The design of these devices requires the accurate modeling of light-matter interactions at the nanoscale and the optimization of multiple design parameters, both of which can be computationally demanding and time intensive. Further, fabrication of these devices demands a high level of accuracy, resolution, and throughput while ideally being able to incorporate multiple materials in complex geometries. To address these considerations in the realization of nanophotonic devices, recent work within our lab has pursued the efficient and accurate modeling of nanoparticles and the assembly of complex 3D micro- and nanostructures using optical tweezers. This Feature Article review highlights these developments as well as related efforts by others in computation and fabrication methods related to nanophotonic devices and metamaterials.
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Affiliation(s)
- Natalie Shultz
- Wyant College of Optical Sciences, University of Arizona, 1630 E University Blvd, Tucson, AZ, USA.
| | - Euan McLeod
- Wyant College of Optical Sciences, University of Arizona, 1630 E University Blvd, Tucson, AZ, USA.
- BIO5 Institute, University of Arizona, 1657 E Helen St, Tucson, AZ, USA
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11
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Zhu Y, Liu R, Yi A, Wang X, Qin Y, Zhao Z, Zhao J, Chen B, Zhang X, Song S, Huo Y, Ou X, Zhang J. A hybrid single quantum dot coupled cavity on a CMOS-compatible SiC photonic chip for Purcell-enhanced deterministic single-photon emission. LIGHT, SCIENCE & APPLICATIONS 2025; 14:86. [PMID: 39952922 PMCID: PMC11828937 DOI: 10.1038/s41377-024-01676-y] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 05/01/2024] [Revised: 10/25/2024] [Accepted: 10/28/2024] [Indexed: 02/17/2025]
Abstract
The ability to control nonclassical light emission from a single quantum emitter by an integrated cavity may unleash new perspectives for integrated photonic quantum applications. However, coupling a single quantum emitter to cavity within photonic circuitry towards creation of the Purcell-enhanced single-photon emission is elusive due to the complexity of integrating active devices in low-loss photonic circuits. Here we demonstrate a hybrid micro-ring resonator (HMRR) coupled with self-assembled quantum dots (QDs) for cavity-enhanced deterministic single-photon emission. The HMRR cavity supports whispering-gallery modes with quality factors up to 7.8×103. By further introducing a micro-heater, we show that the photon emission of QDs can be locally and dynamically tuned over one free spectral ranges of the HMRR ( ~ 4 nm). This allows precise tuning of individual QDs in resonance with the cavity modes, thereby enhancing single-photon emission with a Purcell factor of about 4.9. Our results on the hybrid integrated cavities coupled with two-level quantum emitters emerge as promising devices for chip-based scalable photonic quantum applications.
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Grants
- 16ZR1442600, 20JC1416200 Science and Technology Commission of Shanghai Municipality (Shanghai Municipal Science and Technology Commission)
- 12074400, U1732268, 61874128, 61851406, 11705262, 11774326 National Natural Science Foundation of China (National Science Foundation of China)
- 12074400, U1732268, 62293521, 61874128, 61851406, 11705262, 11774326 National Natural Science Foundation of China (National Science Foundation of China)
- 62293521 National Natural Science Foundation of China (National Science Foundation of China)
- National Key R\&D Program of China (2022YFA1404604)
- Shanghai Municipal Science and Technology Major Project (Grant No. 2019SHZDZX01), Shanghai Science and Technology Innovation Action Plan Program (20JC1416200)
- National Key R\&D Program of China (2022YFA1404604),Chinese Academy of Sciences Project for Young Scientists in Basic Research (No. YSBR-112)
- Frontier Science Key Program of Chinese Academy of Sciences (No. QYZDY-SSW-JSC032)
- Shanghai Science and Technology Innovation Action Plan Program (22JC1403300)
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Affiliation(s)
- Yifan Zhu
- State Key Laboratory of Materials for Integrated Circuits, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, 865 Changning Road, Shanghai, 200050, China
- Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, 100049, China
| | - Runze Liu
- Department of Physics, The Chinese University of Hong Kong, Hong Kong, 999077, China
| | - Ailun Yi
- State Key Laboratory of Materials for Integrated Circuits, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, 865 Changning Road, Shanghai, 200050, China
- Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, 100049, China
| | - Xudong Wang
- State Key Laboratory of Materials for Integrated Circuits, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, 865 Changning Road, Shanghai, 200050, China
- Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, 100049, China
| | - Yuanhao Qin
- State Key Laboratory of Materials for Integrated Circuits, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, 865 Changning Road, Shanghai, 200050, China
- Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, 100049, China
| | - Zihao Zhao
- State Key Laboratory of Materials for Integrated Circuits, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, 865 Changning Road, Shanghai, 200050, China
- Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, 100049, China
| | - Junyi Zhao
- Hefei National Research Center for Physical Sciences, the Microscale and School of Physical Sciences, University of Science and Technology of China, Hefei, 230026, China
- Shanghai Research Center for Quantum Science and CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Shanghai, 201315, China
| | - Bowen Chen
- State Key Laboratory of Materials for Integrated Circuits, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, 865 Changning Road, Shanghai, 200050, China
- Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, 100049, China
| | - Xiuqi Zhang
- State Key Laboratory of Materials for Integrated Circuits, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, 865 Changning Road, Shanghai, 200050, China
- Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, 100049, China
| | - Sannian Song
- State Key Laboratory of Materials for Integrated Circuits, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, 865 Changning Road, Shanghai, 200050, China
- Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, 100049, China
| | - Yongheng Huo
- Hefei National Research Center for Physical Sciences, the Microscale and School of Physical Sciences, University of Science and Technology of China, Hefei, 230026, China.
- Shanghai Research Center for Quantum Science and CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Shanghai, 201315, China.
| | - Xin Ou
- State Key Laboratory of Materials for Integrated Circuits, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, 865 Changning Road, Shanghai, 200050, China.
- Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, 100049, China.
| | - Jiaxiang Zhang
- State Key Laboratory of Materials for Integrated Circuits, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, 865 Changning Road, Shanghai, 200050, China.
- Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, 100049, China.
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12
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Aghaee Rad H, Ainsworth T, Alexander RN, Altieri B, Askarani MF, Baby R, Banchi L, Baragiola BQ, Bourassa JE, Chadwick RS, Charania I, Chen H, Collins MJ, Contu P, D'Arcy N, Dauphinais G, De Prins R, Deschenes D, Di Luch I, Duque S, Edke P, Fayer SE, Ferracin S, Ferretti H, Gefaell J, Glancy S, González-Arciniegas C, Grainge T, Han Z, Hastrup J, Helt LG, Hillmann T, Hundal J, Izumi S, Jaeken T, Jonas M, Kocsis S, Krasnokutska I, Larsen MV, Laskowski P, Laudenbach F, Lavoie J, Li M, Lomonte E, Lopetegui CE, Luey B, Lund AP, Ma C, Madsen LS, Mahler DH, Mantilla Calderón L, Menotti M, Miatto FM, Morrison B, Nadkarni PJ, Nakamura T, Neuhaus L, Niu Z, Noro R, Papirov K, Pesah A, Phillips DS, Plick WN, Rogalsky T, Rortais F, Sabines-Chesterking J, Safavi-Bayat S, Sazhaev E, Seymour M, Rezaei Shad K, Silverman M, Srinivasan SA, Stephan M, Tang QY, Tasker JF, Teo YS, Then RB, Tremblay JE, Tzitrin I, Vaidya VD, Vasmer M, Vernon Z, Villalobos LFSSM, Walshe BW, Weil R, Xin X, Yan X, Yao Y, Zamani Abnili M, Zhang Y. Scaling and networking a modular photonic quantum computer. Nature 2025; 638:912-919. [PMID: 39843755 DOI: 10.1038/s41586-024-08406-9] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 06/25/2024] [Accepted: 11/14/2024] [Indexed: 01/24/2025]
Abstract
Photonics offers a promising platform for quantum computing1-4, owing to the availability of chip integration for mass-manufacturable modules, fibre optics for networking and room-temperature operation of most components. However, experimental demonstrations are needed of complete integrated systems comprising all basic functionalities for universal and fault-tolerant operation5. Here we construct a (sub-performant) scale model of a quantum computer using 35 photonic chips to demonstrate its functionality and feasibility. This combines all the primitive components as discrete, scalable rack-deployed modules networked over fibre-optic interconnects, including 84 squeezers6 and 36 photon-number-resolving detectors furnishing 12 physical qubit modes at each clock cycle. We use this machine, which we name Aurora, to synthesize a cluster state7 entangled across separate chips with 86.4 billion modes, and demonstrate its capability of implementing the foliated distance-2 repetition code with real-time decoding. The key building blocks needed for universality and fault tolerance are demonstrated: heralded synthesis of single-temporal-mode non-Gaussian resource states, real-time multiplexing actuated on photon-number-resolving detection, spatiotemporal cluster-state formation with fibre buffers, and adaptive measurements implemented using chip-integrated homodyne detectors with real-time single-clock-cycle feedforward. We also present a detailed analysis of our architecture's tolerances for optical loss, which is the dominant and most challenging hurdle to crossing the fault-tolerant threshold. This work lays out the path to cross the fault-tolerant threshold and scale photonic quantum computers to the point of addressing useful applications.
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Affiliation(s)
- H Aghaee Rad
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - T Ainsworth
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - R N Alexander
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada.
| | - B Altieri
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - M F Askarani
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - R Baby
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - L Banchi
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - B Q Baragiola
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - J E Bourassa
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - R S Chadwick
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - I Charania
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - H Chen
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - M J Collins
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - P Contu
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - N D'Arcy
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - G Dauphinais
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - R De Prins
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - D Deschenes
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - I Di Luch
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - S Duque
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - P Edke
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - S E Fayer
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - S Ferracin
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - H Ferretti
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - J Gefaell
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - S Glancy
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | | | - T Grainge
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - Z Han
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - J Hastrup
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - L G Helt
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - T Hillmann
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - J Hundal
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - S Izumi
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - T Jaeken
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - M Jonas
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - S Kocsis
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - I Krasnokutska
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - M V Larsen
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - P Laskowski
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - F Laudenbach
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - J Lavoie
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada.
| | - M Li
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - E Lomonte
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - C E Lopetegui
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - B Luey
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - A P Lund
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - C Ma
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - L S Madsen
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - D H Mahler
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | | | - M Menotti
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - F M Miatto
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - B Morrison
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - P J Nadkarni
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - T Nakamura
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - L Neuhaus
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - Z Niu
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - R Noro
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - K Papirov
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - A Pesah
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - D S Phillips
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - W N Plick
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - T Rogalsky
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - F Rortais
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | | | - S Safavi-Bayat
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - E Sazhaev
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - M Seymour
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - K Rezaei Shad
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - M Silverman
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - S A Srinivasan
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - M Stephan
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - Q Y Tang
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - J F Tasker
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - Y S Teo
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - R B Then
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - J E Tremblay
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - I Tzitrin
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - V D Vaidya
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - M Vasmer
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - Z Vernon
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | | | - B W Walshe
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - R Weil
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - X Xin
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - X Yan
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | - Y Yao
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
| | | | - Y Zhang
- Xanadu Quantum Technologies Inc., Toronto, Ontario, Canada
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13
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Huang SY, Barz S. Compact inverse designed vertical coupler with bottom reflector for sub-decibel fiber-to-chip coupling on silicon on insulator platform. Sci Rep 2025; 15:2925. [PMID: 39849000 PMCID: PMC11757707 DOI: 10.1038/s41598-025-86161-1] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 08/09/2024] [Accepted: 01/08/2025] [Indexed: 01/25/2025] Open
Abstract
Inverse design via topology optimization has led to innovations in integrated photonics and offers a promising way for designing high-efficiency on-chip couplers with a minimal footprint. In this work, we exploit topology optimization to design a compact vertical coupler incorporating a bottom reflector, which achieves sub-decibel coupling efficiency on the 220-nm silicon-on-insulator platform. The final design of the vertical coupler yields a predicted coupling efficiency of -0.35 dB at the wavelength of 1550 nm with a footprint of 14 µm × 14 µm, which is considerably smaller than conventional grating couplers. Its topology-optimized geometry can be realized by applying one full-etch and one 70-nm shallow-etch process and the fabricability is also guaranteed by a minimum feature size around 150 nm. Analysis of the potential fabrication imperfections indicates that the topology-optimized coupler is more resilient to in-plane variations, as the deviation of approximately ±100 nm in the misalignment of the topology-optimized features, ±20 nm in the size of the topology-optimized features, and ±10 nm in shallow etch depth yields an additional 1-dB loss as a penalty at the wavelength of 1550 nm. The proposed vertical coupler can further miniaturize photonic integrated circuits and enable highly-efficient networks between optical fibers and other photonic devices.
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Affiliation(s)
- Shiang-Yu Huang
- Institute for Functional Matter and Quantum Technologies, University of Stuttgart, 70569, Stuttgart, Germany.
| | - Stefanie Barz
- Institute for Functional Matter and Quantum Technologies, University of Stuttgart, 70569, Stuttgart, Germany
- Center for Integrated Quantum Science and Technology (IQST), University of Stuttgart, 70569, Stuttgart, Germany
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14
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Gresch A, Kliesch M. Guaranteed efficient energy estimation of quantum many-body Hamiltonians using ShadowGrouping. Nat Commun 2025; 16:689. [PMID: 39814717 PMCID: PMC11735636 DOI: 10.1038/s41467-024-54859-x] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 08/31/2023] [Accepted: 11/22/2024] [Indexed: 01/18/2025] Open
Abstract
Estimation of the energy of quantum many-body systems is a paradigmatic task in various research fields. In particular, efficient energy estimation may be crucial in achieving a quantum advantage for a practically relevant problem. For instance, the measurement effort poses a critical bottleneck for variational quantum algorithms. We aim to find the optimal strategy with single-qubit measurements that yields the highest provable accuracy given a total measurement budget. As a central tool, we establish tail bounds for empirical estimators of the energy. They are helpful for identifying measurement settings that improve the energy estimate the most. This task constitutes an NP-hard problem. However, we are able to circumvent this bottleneck and use the tail bounds to develop a practical, efficient estimation strategy, which we call ShadowGrouping. As the name indicates, it combines shadow estimation methods with grouping strategies for Pauli strings. In numerical experiments, we demonstrate that ShadowGrouping improves upon state-of-the-art methods in estimating the electronic ground-state energies of various small molecules, both in provable and practical accuracy benchmarks. Hence, this work provides a promising way, e.g., to tackle the measurement bottleneck associated with quantum many-body Hamiltonians.
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Affiliation(s)
- Alexander Gresch
- Faculty of Mathematics and Natural Sciences, Heinrich Heine University Düsseldorf, Düsseldorf, Germany.
- Institute for Quantum Inspired and Quantum Optimization, Hamburg University of Technology, Hamburg, Germany.
| | - Martin Kliesch
- Institute for Quantum Inspired and Quantum Optimization, Hamburg University of Technology, Hamburg, Germany.
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15
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Sadeghli Dizaji P, Habibiyan H. Machine learning with knowledge constraints for design optimization of microring resonators as a quantum light source. Sci Rep 2025; 15:372. [PMID: 39748075 PMCID: PMC11697578 DOI: 10.1038/s41598-024-84560-4] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 10/02/2024] [Accepted: 12/24/2024] [Indexed: 01/04/2025] Open
Abstract
With careful design and integration, microring resonators can serve as a promising foundation for developing compact and scalable sources of non-classical light for quantum information processing. However, the current design flow is hindered by computational challenges and a complex, high-dimensional parameter space with interdependent variables. In this work, we present a knowledge-integrated machine learning framework based on Bayesian Optimization for designing squeezed light sources using microring resonators. Our model, after only 5 optimization rounds, identified two optimal structures with distinct cross-sectional areas and radii (65 [Formula: see text] and 110 [Formula: see text]), achieving escape efficiencies over 90% and on-chip squeezing levels of 7.48 dB and 9.86 dB, respectively. Our results demonstrate that by adaptively finding the coupling coefficient through BO, the model has identified optimal points in the over-coupled regions with superior performance. This optimization model is developed specifically for single resonators made of silicon nitride. However, its applicability extends beyond this, and it can be used to model structures with auxiliary rings or other materials like silicon carbide. Our approach is expected to streamline the design of other integrated photonic components, including Mach-Zehnder interferometers and directional couplers, for applications in quantum photonic circuits and optical neural networks.
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Affiliation(s)
- Parisa Sadeghli Dizaji
- Departemant of Physics and Energy Engineering, Amirkabir University of Technology, Tehran, Iran
| | - Hamidreza Habibiyan
- Departemant of Physics and Energy Engineering, Amirkabir University of Technology, Tehran, Iran.
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16
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De Koninck Y, Caer C, Yudistira D, Baryshnikova M, Sar H, Hsieh PY, Özdemir CI, Patra SK, Kuznetsova N, Colucci D, Milenin A, Yimam AA, Morthier G, Van Thourhout D, Verheyen P, Pantouvaki M, Kunert B, Van Campenhout J. GaAs nano-ridge laser diodes fully fabricated in a 300-mm CMOS pilot line. Nature 2025; 637:63-69. [PMID: 39743604 DOI: 10.1038/s41586-024-08364-2] [Citation(s) in RCA: 1] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 07/20/2023] [Accepted: 11/07/2024] [Indexed: 01/04/2025]
Abstract
Silicon photonics is a rapidly developing technology that promises to revolutionize the way we communicate, compute and sense the world1-6. However, the lack of highly scalable, native complementary metal-oxide-semiconductor (CMOS)-integrated light sources is one of the main factors hampering its widespread adoption. Despite considerable progress in hybrid and heterogeneous integration of III-V light sources on silicon7-12, monolithic integration by direct epitaxy of III-V materials remains the pinnacle of cost-effective on-chip light sources. Here we report the electrically driven gallium arsenide (GaAs)-based laser diodes fully fabricated on 300-mm Si wafers in a CMOS pilot manufacturing line based on a new integration approach, nano-ridge engineering. GaAs nano-ridge waveguides with embedded p-i-n diodes and InGaAs quantum wells are grown at high quality on a wafer scale. Room-temperature continuous-wave lasing is demonstrated at wavelengths around 1,020 nm in more than 300 devices across a wafer, with threshold currents as low as 5 mA, output powers beyond 1 mW, laser linewidths down to 46 MHz and laser operation up to 55 °C. These results illustrate the potential of the III-V/Si nano-ridge engineering concept for the monolithic integration of laser diodes in a Si photonics platform, enabling future cost-sensitive high-volume applications in optical sensing, interconnects and beyond.
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Affiliation(s)
| | - Charles Caer
- imec, Leuven, Belgium.
- Centre Suisse d'Electronique et de Microtechnique SA (CSEM), Neuchâtel, Switzerland.
| | | | | | | | | | - Cenk Ibrahim Özdemir
- imec, Leuven, Belgium
- Photonics Research Group, Ghent University-imec, Ghent, Belgium
- Infinera Corporation, Sunnyvale, CA, USA
| | - Saroj Kanta Patra
- imec, Leuven, Belgium
- AMS-OSRAM International GmbH, Regensburg, Germany
| | | | - Davide Colucci
- imec, Leuven, Belgium
- Photonics Research Group, Ghent University-imec, Ghent, Belgium
| | | | | | - Geert Morthier
- Photonics Research Group, Ghent University-imec, Ghent, Belgium
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17
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Penc P, Moca CP, Legeza Ö, Prosen T, Zaránd G, Werner MA. Loss-Induced Quantum Information Jet in an Infinite Temperature Hubbard Chain. PHYSICAL REVIEW LETTERS 2024; 133:190403. [PMID: 39576900 DOI: 10.1103/physrevlett.133.190403] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/19/2024] [Accepted: 10/01/2024] [Indexed: 11/24/2024]
Abstract
Information propagation in the one-dimensional infinite temperature Hubbard model with a dissipative particle sink at the end of a semi-infinite chain is studied. In the strongly interacting limit, the two-site mutual information and the operator entanglement entropy exhibit a rich structure with two propagating information fronts and superimposed interference fringes. A classical reversible cellular automaton model quantitatively captures the transport and the slow, classical part of the correlations but fails to describe the rapidly propagating information jet. The fast quantum jet resembles coherent free particle propagation, with the accompanying long-ranged interference fringes that are exponentially damped by short-ranged spin correlations in the many-body background.
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Affiliation(s)
- Patrik Penc
- Department of Theoretical Physics, Institute of Physics, Budapest University of Technology and Economics, Műegyetem rkp. 3., H-1111 Budapest, Hungary
- HUN-REN-BME Quantum Dynamics and Correlations Research Group, Budapest University of Technology and Economics, Műegyetem rkp. 3., H-1111 Budapest, Hungary
- Strongly Correlated Systems "Lendület" Research Group, HUN-REN Wigner Research Centre for Physics, P.O. Box 49, 1525 Budapest, Hungary
| | | | | | - Tomaž Prosen
- Department of Physics, Faculty of Mathematics and Physics, University of Ljubljana, Jadranska 19, SI-1000 Ljubljana, Slovenia
- Institute for Mathematics, Physics, and Mechanics, Jadranska 19, SI-1000 Ljubljana, Slovenia
| | | | - Miklós Antal Werner
- Department of Theoretical Physics, Institute of Physics, Budapest University of Technology and Economics, Műegyetem rkp. 3., H-1111 Budapest, Hungary
- HUN-REN-BME Quantum Dynamics and Correlations Research Group, Budapest University of Technology and Economics, Műegyetem rkp. 3., H-1111 Budapest, Hungary
- Strongly Correlated Systems 'Lendület" Research Group, HUN-REN Wigner Research Centre for Physics, P.O. Box 49, 1525 Budapest, Hungary
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18
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Monika M, Nosrati F, George A, Sciara S, Fazili R, Marques Muniz AL, Bisianov A, Lo Franco R, Munro WJ, Chemnitz M, Peschel U, Morandotti R. Quantum state processing through controllable synthetic temporal photonic lattices. NATURE PHOTONICS 2024; 19:95-100. [PMID: 39791014 PMCID: PMC11706774 DOI: 10.1038/s41566-024-01546-4] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 01/18/2024] [Accepted: 09/16/2024] [Indexed: 01/12/2025]
Abstract
Quantum walks on photonic platforms represent a physics-rich framework for quantum measurements, simulations and universal computing. Dynamic reconfigurability of photonic circuitry is key to controlling the walk and retrieving its full operation potential. Universal quantum processing schemes based on time-bin encoding in gated fibre loops have been proposed but not demonstrated yet, mainly due to gate inefficiencies. Here we present a scalable quantum processor based on the discrete-time quantum walk of time-bin-entangled photon pairs on synthetic temporal photonic lattices implemented on a coupled fibre-loop system. We utilize this scheme to path-optimize quantum state operations, including the generation of two- and four-level time-bin entanglement and the respective two-photon interference. The design of the programmable temporal photonic lattice enabled us to control the dynamic of the walk, leading to an increase in the coincidence counts and quantum interference measurements without recurring to post-selection. Our results show how temporal synthetic dimensions can pave the way towards efficient quantum information processing, including quantum phase estimation, Boson sampling and the realization of topological phases of matter for high-dimensional quantum systems in a cost-effective, scalable and robust fibre-based setup.
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Affiliation(s)
- Monika Monika
- Institute of Condensed Matter Theory and Optics, Friedrich-Schiller-University, Jena, Germany
- Institut national de la recherche scientifique, Centre Énergie Matériaux Télécommunications, Varennes, Quebec Canada
| | - Farzam Nosrati
- Institut national de la recherche scientifique, Centre Énergie Matériaux Télécommunications, Varennes, Quebec Canada
- Dipartimento di Ingegneria, Università degli Studi di Palermo, Palermo, Italy
| | - Agnes George
- Institut national de la recherche scientifique, Centre Énergie Matériaux Télécommunications, Varennes, Quebec Canada
| | - Stefania Sciara
- Institut national de la recherche scientifique, Centre Énergie Matériaux Télécommunications, Varennes, Quebec Canada
| | - Riza Fazili
- Institut national de la recherche scientifique, Centre Énergie Matériaux Télécommunications, Varennes, Quebec Canada
| | - André Luiz Marques Muniz
- Institute of Condensed Matter Theory and Optics, Friedrich-Schiller-University, Jena, Germany
- Institut national de la recherche scientifique, Centre Énergie Matériaux Télécommunications, Varennes, Quebec Canada
- Fraunhofer Institute for Applied Optics and Precision Engineering, Jena, Germany
| | - Arstan Bisianov
- Institute of Condensed Matter Theory and Optics, Friedrich-Schiller-University, Jena, Germany
- Institut national de la recherche scientifique, Centre Énergie Matériaux Télécommunications, Varennes, Quebec Canada
- Institute of Semiconductor Technology, Technical University of Braunschweig, Braunschweig, Germany
| | - Rosario Lo Franco
- Dipartimento di Ingegneria, Università degli Studi di Palermo, Palermo, Italy
| | - William J. Munro
- Okinawa Institute of Science and Technology Graduate University, Okinawa, Japan
| | - Mario Chemnitz
- Institut national de la recherche scientifique, Centre Énergie Matériaux Télécommunications, Varennes, Quebec Canada
- Leibniz Institute of Photonic Technology, Jena, Germany
- Institute of Applied Optics and Biophysics, Abbe Center of Photonics, Friedrich-Schiller-University, Jena, Germany
| | - Ulf Peschel
- Institute of Condensed Matter Theory and Optics, Friedrich-Schiller-University, Jena, Germany
| | - Roberto Morandotti
- Institut national de la recherche scientifique, Centre Énergie Matériaux Télécommunications, Varennes, Quebec Canada
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19
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AbuGhanem M. Information processing at the speed of light. FRONTIERS OF OPTOELECTRONICS 2024; 17:33. [PMID: 39342550 PMCID: PMC11439970 DOI: 10.1007/s12200-024-00133-3] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 05/28/2024] [Accepted: 08/05/2024] [Indexed: 10/01/2024]
Abstract
In recent years, quantum computing has made significant strides, particularly in light-based technology. The introduction of quantum photonic chips has ushered in an era marked by scalability, stability, and cost-effectiveness, paving the way for innovative possibilities within compact footprints. This article provides a comprehensive exploration of photonic quantum computing, covering key aspects such as encoding information in photons, the merits of photonic qubits, and essential photonic device components including light squeezers, quantum light sources, interferometers, photodetectors, and waveguides. The article also examines photonic quantum communication and internet, and its implications for secure systems, detailing implementations such as quantum key distribution and long-distance communication. Emerging trends in quantum communication and essential reconfigurable elements for advancing photonic quantum internet are discussed. The review further navigates the path towards establishing scalable and fault-tolerant photonic quantum computers, highlighting quantum computational advantages achieved using photons. Additionally, the discussion extends to programmable photonic circuits, integrated photonics and transformative applications. Lastly, the review addresses prospects, implications, and challenges in photonic quantum computing, offering valuable insights into current advancements and promising future directions in this technology.
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20
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Bouchard F, Fenwick K, Bonsma-Fisher K, England D, Bustard PJ, Heshami K, Sussman B. Programmable Photonic Quantum Circuits with Ultrafast Time-Bin Encoding. PHYSICAL REVIEW LETTERS 2024; 133:090601. [PMID: 39270170 DOI: 10.1103/physrevlett.133.090601] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/17/2023] [Accepted: 07/09/2024] [Indexed: 09/15/2024]
Abstract
We propose a quantum information processing platform that utilizes the ultrafast time-bin encoding of photons. This approach offers a pathway to scalability by leveraging the inherent phase stability of collinear temporal interferometric networks at the femtosecond-to-picosecond timescale. The proposed architecture encodes information in ultrafast temporal bins processed using optically induced nonlinearities and birefringent materials while keeping photons in a single spatial mode. We demonstrate the potential for scalable photonic quantum information processing through two independent experiments that showcase the platform's programmability and scalability, respectively. The scheme's programmability is demonstrated in the first experiment, where we successfully program 362 different unitary transformations in up to eight dimensions in a temporal circuit. In the second experiment, we show the scalability of ultrafast time-bin encoding by building a passive optical network, with increasing circuit depth, of up to 36 optical modes. In each experiment, fidelities exceed 97%, while the interferometric phase remains passively stable for several days.
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Affiliation(s)
| | - Kate Fenwick
- National Research Council of Canada, 100 Sussex Drive, Ottawa, Ontario K1A 0R6, Canada
- Department of Physics, University of Ottawa, Advanced Research Complex, 25 Templeton Street, Ottawa, Ontario K1N 6N5, Canada
| | | | | | | | - Khabat Heshami
- National Research Council of Canada, 100 Sussex Drive, Ottawa, Ontario K1A 0R6, Canada
- Department of Physics, University of Ottawa, Advanced Research Complex, 25 Templeton Street, Ottawa, Ontario K1N 6N5, Canada
| | - Benjamin Sussman
- National Research Council of Canada, 100 Sussex Drive, Ottawa, Ontario K1A 0R6, Canada
- Department of Physics, University of Ottawa, Advanced Research Complex, 25 Templeton Street, Ottawa, Ontario K1N 6N5, Canada
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21
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Chen R, Luo YH, Long J, Shi B, Shen C, Liu J. Ultralow-Loss Integrated Photonics Enables Bright, Narrowband, Photon-Pair Sources. PHYSICAL REVIEW LETTERS 2024; 133:083803. [PMID: 39241729 DOI: 10.1103/physrevlett.133.083803] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/28/2024] [Accepted: 07/23/2024] [Indexed: 09/09/2024]
Abstract
Photon-pair sources are critical building blocks for photonic quantum systems. Leveraging Kerr nonlinearity and cavity-enhanced spontaneous four-wave mixing, chip-scale photon-pair sources can be created using microresonators built on photonic integrated circuit. For practical applications, a high microresonator quality factor Q is mandatory to magnify photon-pair sources' brightness and reduce their linewidth. The former is proportional to Q^{4}, while the latter is inversely proportional to Q. Here, we demonstrate an integrated, microresonator-based, narrowband photon-pair source. The integrated microresonator, made of silicon nitride and fabricated using a standard CMOS foundry process, features ultralow loss down to 0.03 dB/cm and intrinsic Q factor exceeding 10^{7}. The photon-pair source has brightness of 1.17×10^{9} Hz/mW^{2}/GHz and linewidth of 25.9 MHz, both of which are record values for silicon-photonics-based quantum light source. It further enables a heralded single-photon source with heralded second-order correlation g_{h}^{(2)}(0)=0.0037(5), as well as an energy-time entanglement source with a raw visibility of 0.973(9). Our work evidences the global potential of ultralow-loss integrated photonics to create novel quantum light sources and circuits, catalyzing efficient, compact, and robust interfaces to quantum communication and networks.
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Affiliation(s)
| | - Yi-Han Luo
- International Quantum Academy, Shenzhen 518048, China
| | - Jinbao Long
- International Quantum Academy, Shenzhen 518048, China
| | | | - Chen Shen
- International Quantum Academy, Shenzhen 518048, China
- Qaleido Photonics, Shenzhen 518048, China
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22
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Zhang ZY, Hu JR, Fang YY, Li JF, Liu JM, Huang X, Sun Z. Quantum gate control of polar molecules with machine learning. J Chem Phys 2024; 161:034102. [PMID: 39007369 DOI: 10.1063/5.0216013] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 04/27/2024] [Accepted: 06/26/2024] [Indexed: 07/16/2024] Open
Abstract
We propose a scheme for achieving basic quantum gates using ultracold polar molecules in pendular states. The qubits are encoded in the YbF molecules trapped in an electric field with a certain gradient and coupled by the dipole-dipole interaction. The time-dependent control sequences consisting of multiple pulses are considered to interact with the pendular qubits. To achieve high-fidelity quantum gates, we map the control problem for the coupled molecular system into a Markov decision process and deal with it using the techniques of deep reinforcement learning (DRL). By training the agents over multiple episodes, the optimal control pulse sequences for the two-qubit gates of NOT, controlled NOT, and Hadamard are discovered with high fidelities. Moreover, the population dynamics of YbF molecules driven by the discovered gate sequences are analyzed in detail. Furthermore, by combining the optimal gate sequences, we successfully simulate the quantum circuit for entanglement. Our findings could offer new insights into efficiently controlling molecular systems for practical molecule-based quantum computing using DRL.
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Affiliation(s)
- Zuo-Yuan Zhang
- College of Physical Science and Technology, Yangzhou University, Yangzhou 225009, China
| | - Jie-Ru Hu
- State Key Laboratory of Precision Spectroscopy, School of Physics and Electronic Science, East China Normal University, Shanghai 200241, China
| | - Yu-Yan Fang
- State Key Laboratory of Precision Spectroscopy, School of Physics and Electronic Science, East China Normal University, Shanghai 200241, China
| | - Jin-Fang Li
- Department of Physics and Electronic Engineering, Xianyang Normal University, Shaanxi 712000, China
| | - Jin-Ming Liu
- State Key Laboratory of Precision Spectroscopy, School of Physics and Electronic Science, East China Normal University, Shanghai 200241, China
- Chongqing Key Laboratory of Precision Optics, Chongqing Institute of East China Normal University, Chongqing 401120, China
| | - Xinning Huang
- College of Physical Science and Technology, Yangzhou University, Yangzhou 225009, China
| | - Zhaoxi Sun
- Changping Laboratory, Beijing 102206, China
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23
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Zhu HH, Sen Chen H, Chen T, Li Y, Luo SB, Karim MF, Luo XS, Gao F, Li Q, Cai H, Chin LK, Kwek LC, Nordén B, Zhang XD, Liu AQ. Large-scale photonic network with squeezed vacuum states for molecular vibronic spectroscopy. Nat Commun 2024; 15:6057. [PMID: 39025843 PMCID: PMC11258230 DOI: 10.1038/s41467-024-50060-2] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 08/01/2023] [Accepted: 06/28/2024] [Indexed: 07/20/2024] Open
Abstract
Although molecular vibronic spectra generation is pivotal for chemical analysis, tackling such exponentially complex tasks on classical computers remains inefficient. Quantum simulation, though theoretically promising, faces technological challenges in experimentally extracting vibronic spectra for molecules with multiple modes. Here, we propose a nontrivial algorithm to generate the vibronic spectra using states with zero displacements (squeezed vacuum states) coupled to a linear optical network, offering ease of experimental implementation. We also fabricate an integrated quantum photonic microprocessor chip as a versatile simulation platform containing 16 modes of single-mode squeezed vacuum states and a fully programmable interferometer network. Molecular vibronic spectra of formic acid and thymine under the Condon approximation are simulated using the quantum microprocessor chip with high reconstructed fidelity ( > 92%). Furthermore, vibronic spectra of naphthalene, phenanthrene, and benzene under the non-Condon approximation are also experimentally simulated. Such demonstrations could pave the way for solving complicated quantum chemistry problems involving vibronic spectra and computational tasks beyond the reach of classical computers.
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Affiliation(s)
- Hui Hui Zhu
- Quantum Science and Engineering Centre (QSec), Nanyang Technological University, Singapore, Singapore
| | - Hao Sen Chen
- Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurements of Ministry of Education, School of Physics, Beijing Institute of Technology, Beijing, China
| | - Tian Chen
- Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurements of Ministry of Education, School of Physics, Beijing Institute of Technology, Beijing, China.
| | - Yuan Li
- Quantum Science and Engineering Centre (QSec), Nanyang Technological University, Singapore, Singapore
| | - Shao Bo Luo
- School of Microelectronics, Southern University of Science and Technology, Shenzhen, China
| | - Muhammad Faeyz Karim
- Quantum Science and Engineering Centre (QSec), Nanyang Technological University, Singapore, Singapore
| | | | - Feng Gao
- Advanced Micro Foundry, Singapore, Singapore
| | - Qiang Li
- Advanced Micro Foundry, Singapore, Singapore
| | - Hong Cai
- Institute of Microelectronics, A*STAR (Agency for Science, Technology, and Research), Singapore, Singapore
| | - Lip Ket Chin
- Department of Electrical Engineering, City University of Hong Kong, Hong Kong SAR, China.
| | - Leong Chuan Kwek
- Quantum Science and Engineering Centre (QSec), Nanyang Technological University, Singapore, Singapore.
- Centre for Quantum Technologies, National University of Singapore, Singapore, Singapore.
| | - Bengt Nordén
- Department of Chemistry and Chemical Engineering, Chalmers University of Technology, Gothenburg, Sweden.
| | - Xiang Dong Zhang
- Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurements of Ministry of Education, School of Physics, Beijing Institute of Technology, Beijing, China.
| | - Ai Qun Liu
- Quantum Science and Engineering Centre (QSec), Nanyang Technological University, Singapore, Singapore.
- Institute of Quantum Technology (IQT), The Hong Kong Polytechnic University, Hong Kong SAR, China.
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24
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Borghi M, Pagano PL, Liscidini M, Bajoni D, Galli M. Uncorrelated photon pair generation from an integrated silicon nitride resonator measured by time-resolved coincidence detection. OPTICS LETTERS 2024; 49:3966-3969. [PMID: 39008757 DOI: 10.1364/ol.527965] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/25/2024] [Accepted: 06/19/2024] [Indexed: 07/17/2024]
Abstract
We measure the joint temporal intensity of signal and idler photon pairs generated by spontaneous four-wave mixing in a silicon nitride microresonator by time-resolved coincidence detection. This technique can be applied to any high-Q optical cavity whose photon lifetime exceeds the duration of the pump pulse. We tailor the temporal correlation of photon pairs by using a resonant interferometric coupler, a device that allows us to independently tune the quality factors of the pump and signal and idler resonances. Temporal post-selection is used to accurately measure the temporal emission of the device, demonstrating a purity of 98.67(1)%.
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25
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Ehrhardt M, Dittel C, Heinrich M, Szameit A. Topological Hong-Ou-Mandel interference. Science 2024; 384:1340-1344. [PMID: 38900876 DOI: 10.1126/science.ado8192] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 02/24/2024] [Accepted: 05/03/2024] [Indexed: 06/22/2024]
Abstract
The interplay of topology and optics provides a route to pursue robust photonic devices, with the application to photonic quantum computation in its infancy. However, the possibilities of harnessing topological structures to process quantum information with linear optics, through the quantum interference of photons, remain largely uncharted. Here, we present a Hong-Ou-Mandel interference effect of topological origin. We show that this interference of photon pairs-ranging from constructive to destructive-is solely determined by a synthetic magnetic flux, rendering it resilient to errors on a fundamental level. Our implementation establishes a quantized flux that facilitates exclusively destructive quantum interference. Our findings pave the way toward the development of next-generation photonic quantum circuitry and scalable quantum computing protected by virtue of topologically robust quantum gates.
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Affiliation(s)
- Max Ehrhardt
- University of Rostock, Institute of Physics, Albert-Einstein-Str. 23, 18059 Rostock, Germany
| | - Christoph Dittel
- Physikalisches Institut, Albert-Ludwigs-Universität Freiburg, Hermann-Herder-Str. 3, 79104 Freiburg, Germany
- EUCOR Centre for Quantum Science and Quantum Computing, Albert-Ludwigs-Universität Freiburg, Hermann-Herder-Str. 3, 79104 Freiburg, Germany
| | - Matthias Heinrich
- University of Rostock, Institute of Physics, Albert-Einstein-Str. 23, 18059 Rostock, Germany
| | - Alexander Szameit
- University of Rostock, Institute of Physics, Albert-Einstein-Str. 23, 18059 Rostock, Germany
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26
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Moridsadat M, Tamura M, Chrostowski L, Shekhar S, Shastri BJ. Physics to system-level modeling of silicon-organic-hybrid nanophotonic devices. Sci Rep 2024; 14:11751. [PMID: 38782947 PMCID: PMC11116435 DOI: 10.1038/s41598-024-61618-x] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 01/19/2024] [Accepted: 05/07/2024] [Indexed: 05/25/2024] Open
Abstract
The continuous growth in data volume has sparked interest in silicon-organic-hybrid (SOH) nanophotonic devices integrated into silicon photonic integrated circuits (PICs). SOH devices offer improved speed and energy efficiency compared to silicon photonics devices. However, a comprehensive and accurate modeling methodology of SOH devices, such as modulators corroborating experimental results, is lacking. While some preliminary modeling approaches for SOH devices exist, their reliance on theoretical and numerical methodologies, along with a lack of compatibility with electronic design automation (EDA), hinders their seamless and rapid integration with silicon PICs. Here, we develop a phenomenological, building-block-based SOH PICs simulation methodology that spans from the physics to the system level, offering high accuracy, comprehensiveness, and EDA-style compatibility. Our model is also readily integrable and scalable, lending itself to the design of large-scale silicon PICs. Our proposed modeling methodology is agnostic and compatible with any photonics-electronics co-simulation software. We validate this methodology by comparing the characteristics of experimentally demonstrated SOH microring modulators (MRMs) and Mach Zehnder modulators with those obtained through simulation, demonstrating its ability to model various modulator topologies. We also show our methodology's ease and speed in modeling large-scale systems. As an illustrative example, we use our methodology to design and study a 3-channel SOH MRM-based wavelength-division (de)multiplexer, a widely used component in various applications, including neuromorphic computing, data center interconnects, communications, sensing, and switching networks. Our modeling approach is also compatible with other materials exhibiting the Pockels and Kerr effects. To our knowledge, this represents the first comprehensive physics-to-system-level EDA-compatible simulation methodology for SOH modulators.
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Affiliation(s)
- Maryam Moridsadat
- Department of Physics, Center of Nanophotonics, Engineering Physics and Astronomy, Queen's University, 64 Bader Lane, Kingston, ON, K7L 3N6, Canada.
| | - Marcus Tamura
- Department of Physics, Center of Nanophotonics, Engineering Physics and Astronomy, Queen's University, 64 Bader Lane, Kingston, ON, K7L 3N6, Canada
| | - Lukas Chrostowski
- Department of Electrical and Computer Engineering, University of British Columbia, Vancouver, BC, V6T 1Z4, Canada
| | - Sudip Shekhar
- Department of Electrical and Computer Engineering, University of British Columbia, Vancouver, BC, V6T 1Z4, Canada
| | - Bhavin J Shastri
- Department of Physics, Center of Nanophotonics, Engineering Physics and Astronomy, Queen's University, 64 Bader Lane, Kingston, ON, K7L 3N6, Canada.
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27
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Carosini L, Oddi V, Giorgino F, Hansen LM, Seron B, Piacentini S, Guggemos T, Agresti I, Loredo JC, Walther P. Programmable multiphoton quantum interference in a single spatial mode. SCIENCE ADVANCES 2024; 10:eadj0993. [PMID: 38640248 DOI: 10.1126/sciadv.adj0993] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/06/2023] [Accepted: 03/18/2024] [Indexed: 04/21/2024]
Abstract
The interference of nonclassical states of light enables quantum-enhanced applications reaching from metrology to computation. Most commonly, the polarization or spatial location of single photons are used as addressable degrees of freedom for turning these applications into praxis. However, the scale-up for the processing of a large number of photons of these architectures is very resource-demanding due to the rapidly increasing number of components, such as optical elements, photon sources, and detectors. Here, we demonstrate a resource-efficient architecture for multiphoton processing based on time-bin encoding in a single spatial mode. We use an efficient quantum dot single-photon source and a fast programmable time-bin interferometer to observe the interference of up to eight photons in 16 modes, all recorded only with one detector, thus considerably reducing the physical overhead previously needed for achieving equivalent tasks. Our results can form the basis for a future universal photonics quantum processor operating in a single spatial mode.
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Affiliation(s)
- Lorenzo Carosini
- University of Vienna, Faculty of Physics,Vienna Center for Quantum Science and Technology (VCQ), 1090 Vienna, Austria
- Christian Doppler Laboratory for Photonic Quantum Computer, Faculty of Physics, University of Vienna, 1090 Vienna, Austria
| | - Virginia Oddi
- Dipartimento di Fisica, Politecnico di Milano, Piazza Leonardo da Vinci, 32, I-20133 Milano, Italy
| | - Francesco Giorgino
- University of Vienna, Faculty of Physics,Vienna Center for Quantum Science and Technology (VCQ), 1090 Vienna, Austria
- Christian Doppler Laboratory for Photonic Quantum Computer, Faculty of Physics, University of Vienna, 1090 Vienna, Austria
| | - Lena M Hansen
- University of Vienna, Faculty of Physics,Vienna Center for Quantum Science and Technology (VCQ), 1090 Vienna, Austria
- Christian Doppler Laboratory for Photonic Quantum Computer, Faculty of Physics, University of Vienna, 1090 Vienna, Austria
| | - Benoit Seron
- Quantum Information and Communication, Ecole polytechnique de Bruxelles, CP 165/59, Université libre de Bruxelles (ULB), 1050 Brussels, Belgium
| | - Simone Piacentini
- Dipartimento di Fisica, Politecnico di Milano, Piazza Leonardo da Vinci, 32, I-20133 Milano, Italy
- Istituto di Fotonica e Nanotecnologie, Consiglio Nazionale delle Ricerche (IFN-CNR), Piazza Leonardo da Vinci, 32, I-20133 Milano, Italy
| | - Tobias Guggemos
- University of Vienna, Faculty of Physics,Vienna Center for Quantum Science and Technology (VCQ), 1090 Vienna, Austria
- Christian Doppler Laboratory for Photonic Quantum Computer, Faculty of Physics, University of Vienna, 1090 Vienna, Austria
- Remote Sensing Technology Institute, German Aerospace Center DLR, Münchener Straße 20, 82234 Weßling, Germany
| | - Iris Agresti
- University of Vienna, Faculty of Physics,Vienna Center for Quantum Science and Technology (VCQ), 1090 Vienna, Austria
| | - Juan C Loredo
- University of Vienna, Faculty of Physics,Vienna Center for Quantum Science and Technology (VCQ), 1090 Vienna, Austria
- Christian Doppler Laboratory for Photonic Quantum Computer, Faculty of Physics, University of Vienna, 1090 Vienna, Austria
| | - Philip Walther
- University of Vienna, Faculty of Physics,Vienna Center for Quantum Science and Technology (VCQ), 1090 Vienna, Austria
- Christian Doppler Laboratory for Photonic Quantum Computer, Faculty of Physics, University of Vienna, 1090 Vienna, Austria
- University of Vienna, Research Network for Quantum Aspects of Space Time (TURIS), Boltzmanngasse 5, 1090 Vienna, Austria
- Institute for Quantum Optics and Quantum Information (IQOQI) Vienna, Austrian Academy of Sciences, Boltzmanngasse 3, 1090 Vienna, Austria
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28
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Yard P, Jones AE, Paesani S, Maïnos A, Bulmer JFF, Laing A. On-Chip Quantum Information Processing with Distinguishable Photons. PHYSICAL REVIEW LETTERS 2024; 132:150602. [PMID: 38682995 DOI: 10.1103/physrevlett.132.150602] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/18/2022] [Accepted: 11/07/2023] [Indexed: 05/01/2024]
Abstract
Multiphoton interference is at the heart of photonic quantum technologies. Arrays of integrated cavities can support bright sources of single photons with high purity and small footprint, but the inevitable spectral distinguishability between photons generated from nonidentical cavities is an obstacle to scaling. In principle, this problem can be alleviated by measuring photons with high timing resolution, which erases spectral information through the time-energy uncertainty relation. Here, we experimentally demonstrate that detection can be implemented with a temporal resolution sufficient to interfere photons detuned on the scales necessary for cavity-based integrated photon sources. By increasing the effective timing resolution of the system from 200 to 20 ps, we observe a 20% increase in the visibility of quantum interference between independent photons from integrated microring resonator sources that are detuned by 6.8 GHz. We go on to show how time-resolved detection of nonideal photons can be used to improve the fidelity of an entangling operation and to mitigate the reduction of computational complexity in boson sampling experiments. These results pave the way for photonic quantum information processing with many photon sources without the need for active alignment.
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Affiliation(s)
- Patrick Yard
- Quantum Engineering and Technology Laboratories, School of Physics and Department of Electrical and Electronic Engineering, University of Bristol, Bristol, United Kingdom
| | - Alex E Jones
- Quantum Engineering and Technology Laboratories, School of Physics and Department of Electrical and Electronic Engineering, University of Bristol, Bristol, United Kingdom
| | - Stefano Paesani
- Quantum Engineering and Technology Laboratories, School of Physics and Department of Electrical and Electronic Engineering, University of Bristol, Bristol, United Kingdom
- Center for Hybrid Quantum Networks (Hy-Q), Niels Bohr Institute, University of Copenhagen, Blegdamsvej 17, DK-2100 Copenhagen, Denmark
| | - Alexandre Maïnos
- Quantum Engineering and Technology Laboratories, School of Physics and Department of Electrical and Electronic Engineering, University of Bristol, Bristol, United Kingdom
| | - Jacob F F Bulmer
- Quantum Engineering and Technology Laboratories, School of Physics and Department of Electrical and Electronic Engineering, University of Bristol, Bristol, United Kingdom
| | - Anthony Laing
- Quantum Engineering and Technology Laboratories, School of Physics and Department of Electrical and Electronic Engineering, University of Bristol, Bristol, United Kingdom
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29
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Jabri H, Eleuch H. Light squeezing enhancement by coupling nonlinear optical cavities. Sci Rep 2024; 14:7753. [PMID: 38565597 PMCID: PMC10987607 DOI: 10.1038/s41598-024-58447-3] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 01/17/2024] [Accepted: 03/29/2024] [Indexed: 04/04/2024] Open
Abstract
In this paper, we explore the squeezing effect generated by two coupled optical cavities. Each cavity contains a second-order nonlinear material and coherently pumped by a laser. Our results show that light intensity is strongly improved due to the presence of the nonlinearities and mainly depends on the detunings between external laser frequencies and cavity modes. More interestingly, the proposed scheme could enhance light squeezing for moderate coupling between cavities : the squeezing generated by one cavity is enhanced by the other one. For resonant interaction, highest squeezing effect is obtained near resonance. When fields are non resonant, squeezing increases near resonance of the considered cavity, but decreases for large detunings relative to the second cavity. Further, when the dissipation rate of the second cavity is smaller than the first, the squeezing could be improved, attaining nearly the perfect squeezing. While the temperature elevation has a negative impact overall on the nonclassical light, squeezing shows an appreciable resistance against thermal baths for appropriate parameter sets.
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Affiliation(s)
- H Jabri
- Higher Institute of Biotechnology of Beja, University of Jendouba, Beja, 9000, Tunisia.
| | - H Eleuch
- Department of Applied Physics and Astronomy, University of Sharjah, Sharjah, 27272, United Arab Emirates
- College of Arts and Sciences, Abu Dhabi University, Abu Dhabi, 59911, United Arab Emirates
- Institute for Quantum Science and Engineering, Texas A&M University, College Station, TX 77843, USA
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30
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Yang TY, Wang XB. Speeding up the classical simulation of Gaussian boson sampling with limited connectivity. Sci Rep 2024; 14:7680. [PMID: 38561440 PMCID: PMC10984997 DOI: 10.1038/s41598-024-58136-1] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 12/15/2023] [Accepted: 03/26/2024] [Indexed: 04/04/2024] Open
Abstract
Gaussian boson sampling (GBS) plays a crucially important role in demonstrating quantum advantage. As a major imperfection, the limited connectivity of the linear optical network weakens the quantum advantage result in recent experiments. In this work, we introduce an enhanced classical algorithm for simulating GBS processes with limited connectivity. It computes the loop Hafnian of an n × n symmetric matrix with bandwidth w in O ( n w 2 w ) time. It is better than the previous fastest algorithm which runs in O ( n w 2 2 w ) time. This classical algorithm is helpful on clarifying how limited connectivity affects the computational complexity of GBS and tightening the boundary for achieving quantum advantage in the GBS problem.
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Affiliation(s)
- Tian-Yu Yang
- State Key Laboratory of Low Dimensional Quantum Physics, Department of Physics, Tsinghua University, Beijing, 100084, China
| | - Xiang-Bin Wang
- State Key Laboratory of Low Dimensional Quantum Physics, Department of Physics, Tsinghua University, Beijing, 100084, China.
- Jinan Institute of Quantum Technology, SAICT, Jinan, 250101, China.
- Shanghai Branch, CAS Center for Excellence and Synergetic Innovation Center in Quantum Information and Quantum Physics, University of Science and Technology of China, Shanghai, 201315, China.
- International Quantum Academy, Shenzhen, 518048, China.
- Frontier Science Center for Quantum Information, Beijing, 100084, China.
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31
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Zeng H, He ZQ, Fan YR, Luo Y, Lyu C, Wu JP, Li YB, Liu S, Wang D, Zhang DC, Zeng JJ, Deng GW, Wang Y, Song HZ, Wang Z, You LX, Guo K, Sun CZ, Luo Y, Guo GC, Zhou Q. Quantum Light Generation Based on GaN Microring toward Fully On-Chip Source. PHYSICAL REVIEW LETTERS 2024; 132:133603. [PMID: 38613308 DOI: 10.1103/physrevlett.132.133603] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/19/2023] [Revised: 12/12/2023] [Accepted: 01/29/2024] [Indexed: 04/14/2024]
Abstract
An integrated quantum light source is increasingly desirable in large-scale quantum information processing. Despite recent remarkable advances, a new material platform is constantly being explored for the fully on-chip integration of quantum light generation, active and passive manipulation, and detection. Here, for the first time, we demonstrate a gallium nitride (GaN) microring based quantum light generation in the telecom C-band, which has potential toward the monolithic integration of quantum light source. In our demonstration, the GaN microring has a free spectral range of 330 GHz and a near-zero anomalous dispersion region of over 100 nm. The generation of energy-time entangled photon pair is demonstrated with a typical raw two-photon interference visibility of 95.5±6.5%, which is further configured to generate a heralded single photon with a typical heralded second-order autocorrelation g_{H}^{(2)}(0) of 0.045±0.001. Our results pave the way for developing a chip-scale quantum photonic circuit.
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Affiliation(s)
- Hong Zeng
- Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 611731, China
- Key Laboratory of Quantum Physics and Photonic Quantum Information, Ministry of Education, University of Electronic Science and Technology of China, Chengdu 611731, China
| | - Zhao-Qin He
- Department of Electronic Engineering, Tsinghua University, Beijing 100084, China
| | - Yun-Ru Fan
- Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 611731, China
- Key Laboratory of Quantum Physics and Photonic Quantum Information, Ministry of Education, University of Electronic Science and Technology of China, Chengdu 611731, China
| | - Yue Luo
- Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 611731, China
| | - Chen Lyu
- Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 611731, China
| | - Jin-Peng Wu
- Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 611731, China
- Key Laboratory of Quantum Physics and Photonic Quantum Information, Ministry of Education, University of Electronic Science and Technology of China, Chengdu 611731, China
| | - Yun-Bo Li
- Department of Fundamental Network Technology, China Mobile Research Institute, Beijing 100053, China
| | - Sheng Liu
- Department of Fundamental Network Technology, China Mobile Research Institute, Beijing 100053, China
| | - Dong Wang
- Department of Fundamental Network Technology, China Mobile Research Institute, Beijing 100053, China
| | - De-Chao Zhang
- Department of Fundamental Network Technology, China Mobile Research Institute, Beijing 100053, China
| | - Juan-Juan Zeng
- Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 611731, China
- Center for Quantum Internet, Tianfu Jiangxi Laboratory, Chengdu 641419, China
| | - Guang-Wei Deng
- Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 611731, China
- Key Laboratory of Quantum Physics and Photonic Quantum Information, Ministry of Education, University of Electronic Science and Technology of China, Chengdu 611731, China
| | - You Wang
- Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 611731, China
- Southwest Institute of Technical Physics, Chengdu 610041, China
| | - Hai-Zhi Song
- Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 611731, China
- Southwest Institute of Technical Physics, Chengdu 610041, China
| | - Zhen Wang
- National Key Laboratory of Materials for Integrated Circuits, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, Shanghai 200050, China
| | - Li-Xing You
- National Key Laboratory of Materials for Integrated Circuits, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, Shanghai 200050, China
| | - Kai Guo
- Institute of Systems Engineering, AMS, Beijing 100141, China
| | - Chang-Zheng Sun
- Department of Electronic Engineering, Tsinghua University, Beijing 100084, China
| | - Yi Luo
- Department of Electronic Engineering, Tsinghua University, Beijing 100084, China
| | - Guang-Can Guo
- Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 611731, China
- Key Laboratory of Quantum Physics and Photonic Quantum Information, Ministry of Education, University of Electronic Science and Technology of China, Chengdu 611731, China
- Center for Quantum Internet, Tianfu Jiangxi Laboratory, Chengdu 641419, China
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei 230026, China
| | - Qiang Zhou
- Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 611731, China
- Key Laboratory of Quantum Physics and Photonic Quantum Information, Ministry of Education, University of Electronic Science and Technology of China, Chengdu 611731, China
- Center for Quantum Internet, Tianfu Jiangxi Laboratory, Chengdu 641419, China
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei 230026, China
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32
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Park T, Stokowski H, Ansari V, Gyger S, Multani KKS, Celik OT, Hwang AY, Dean DJ, Mayor F, McKenna TP, Fejer MM, Safavi-Naeini A. Single-mode squeezed-light generation and tomography with an integrated optical parametric oscillator. SCIENCE ADVANCES 2024; 10:eadl1814. [PMID: 38478618 PMCID: PMC10936947 DOI: 10.1126/sciadv.adl1814] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 10/03/2023] [Accepted: 02/08/2024] [Indexed: 03/17/2024]
Abstract
Quantum optical technologies promise advances in sensing, computing, and communication. A key resource is squeezed light, where quantum noise is redistributed between optical quadratures. We introduce a monolithic, chip-scale platform that exploits the χ(2) nonlinearity of a thin-film lithium niobate (TFLN) resonator device to efficiently generate squeezed states of light. Our system integrates all essential components-except for the laser and two detectors-on a single chip with an area of one square centimeter, reducing the size, operational complexity, and power consumption associated with conventional setups. Using the balanced homodyne measurement subsystem that we implemented on the same chip, we measure a squeezing of 0.55 decibels and an anti-squeezing of 1.55 decibels. We use 20 milliwatts of input power to generate the parametric oscillator pump field by using second harmonic generation on the same chip. Our work represents a step toward compact and efficient quantum optical systems posed to leverage the rapid advances in integrated nonlinear and quantum photonics.
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Affiliation(s)
- Taewon Park
- Department of Applied Physics and Ginzton Laboratory, Stanford University, Stanford, CA 94305, USA
- Department of Electrical Engineering, Stanford University, Stanford, CA 94305, USA
| | - Hubert Stokowski
- Department of Applied Physics and Ginzton Laboratory, Stanford University, Stanford, CA 94305, USA
| | - Vahid Ansari
- Department of Applied Physics and Ginzton Laboratory, Stanford University, Stanford, CA 94305, USA
| | - Samuel Gyger
- Department of Applied Physics and Ginzton Laboratory, Stanford University, Stanford, CA 94305, USA
| | - Kevin K. S. Multani
- Department of Applied Physics and Ginzton Laboratory, Stanford University, Stanford, CA 94305, USA
- Department of Physics, Stanford University, Stanford, CA 94305, USA
| | - Oguz Tolga Celik
- Department of Applied Physics and Ginzton Laboratory, Stanford University, Stanford, CA 94305, USA
- Department of Electrical Engineering, Stanford University, Stanford, CA 94305, USA
| | - Alexander Y. Hwang
- Department of Applied Physics and Ginzton Laboratory, Stanford University, Stanford, CA 94305, USA
| | - Devin J. Dean
- Department of Applied Physics and Ginzton Laboratory, Stanford University, Stanford, CA 94305, USA
| | - Felix Mayor
- Department of Applied Physics and Ginzton Laboratory, Stanford University, Stanford, CA 94305, USA
| | - Timothy P. McKenna
- Physics and Informatics Laboratories, NTT Research Inc., Sunnyvale, CA 94085, USA
| | - Martin M. Fejer
- Department of Applied Physics and Ginzton Laboratory, Stanford University, Stanford, CA 94305, USA
| | - Amir Safavi-Naeini
- Department of Applied Physics and Ginzton Laboratory, Stanford University, Stanford, CA 94305, USA
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33
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Yu S, Liu W, Tao SJ, Li ZP, Wang YT, Zhong ZP, Patel RB, Meng Y, Yang YZ, Wang ZA, Guo NJ, Zeng XD, Chen Z, Xu L, Zhang N, Liu X, Yang M, Zhang WH, Zhou ZQ, Xu JS, Tang JS, Han YJ, Li CF, Guo GC. A von-Neumann-like photonic processor and its application in studying quantum signature of chaos. LIGHT, SCIENCE & APPLICATIONS 2024; 13:74. [PMID: 38485915 PMCID: PMC10940704 DOI: 10.1038/s41377-024-01413-5] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 09/05/2023] [Revised: 02/06/2024] [Accepted: 02/17/2024] [Indexed: 03/18/2024]
Abstract
Photonic quantum computation plays an important role and offers unique advantages. Two decades after the milestone work of Knill-Laflamme-Milburn, various architectures of photonic processors have been proposed, and quantum advantage over classical computers has also been demonstrated. It is now the opportune time to apply this technology to real-world applications. However, at current technology level, this aim is restricted by either programmability in bulk optics or loss in integrated optics for the existing architectures of processors, for which the resource cost is also a problem. Here we present a von-Neumann-like architecture based on temporal-mode encoding and looped structure on table, which is capable of multimode-universal programmability, resource-efficiency, phase-stability and software-scalability. In order to illustrate these merits, we execute two different programs with varying resource requirements on the same processor, to investigate quantum signature of chaos from two aspects: the signature behaviors exhibited in phase space (13 modes), and the Fermi golden rule which has not been experimentally studied in quantitative way before (26 modes). The maximal program contains an optical interferometer network with 1694 freely-adjustable phases. Considering current state-of-the-art, our architecture stands as the most promising candidate for real-world applications.
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Affiliation(s)
- Shang Yu
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China
- Research Center for Quantum Sensing, Zhejiang Lab, Hangzhou, 310000, China
- Quantum Optics and Laser Science, Blackett Laboratory, Imperial College London, Prince Consort Rd, London, SW7 2AZ, UK
| | - Wei Liu
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China
| | - Si-Jing Tao
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China
| | - Zhi-Peng Li
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China
| | - Yi-Tao Wang
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China
| | - Zhi-Peng Zhong
- Research Center for Quantum Sensing, Zhejiang Lab, Hangzhou, 310000, China
| | - Raj B Patel
- Quantum Optics and Laser Science, Blackett Laboratory, Imperial College London, Prince Consort Rd, London, SW7 2AZ, UK
- Clarendon Laboratory, Department of Physics, Oxford University, Parks Road OX1 3PU, Oxford, UK
| | - Yu Meng
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China
| | - Yuan-Ze Yang
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China
| | - Zhao-An Wang
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China
| | - Nai-Jie Guo
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China
| | - Xiao-Dong Zeng
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China
| | - Zhe Chen
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China
| | - Liang Xu
- Research Center for Quantum Sensing, Zhejiang Lab, Hangzhou, 310000, China
| | - Ning Zhang
- Research Center for Quantum Sensing, Zhejiang Lab, Hangzhou, 310000, China
| | - Xiao Liu
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China
| | - Mu Yang
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China
| | - Wen-Hao Zhang
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China
| | - Zong-Quan Zhou
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China
| | - Jin-Shi Xu
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China
| | - Jian-Shun Tang
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China.
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China.
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China.
| | - Yong-Jian Han
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China.
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China.
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China.
| | - Chuan-Feng Li
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China.
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China.
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China.
| | - Guang-Can Guo
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China
- CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, 230026, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, 230088, China
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34
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Liu T, Bai K, Zhang Y, Wan D, Lai Y, Chan CT, Xiao M. Finite barrier bound state. LIGHT, SCIENCE & APPLICATIONS 2024; 13:69. [PMID: 38453882 PMCID: PMC10920789 DOI: 10.1038/s41377-024-01417-1] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/29/2023] [Revised: 01/18/2024] [Accepted: 02/26/2024] [Indexed: 03/09/2024]
Abstract
A boundary mode localized on one side of a finite-size lattice can tunnel to the opposite side which results in unwanted couplings. Conventional wisdom tells that the tunneling probability decays exponentially with the size of the system which thus requires many lattice sites before eventually becoming negligibly small. Here we show that the tunneling probability for some boundary modes can apparently vanish at specific wavevectors. Thus, similar to bound states in the continuum, a boundary mode can be completely trapped within very few lattice sites where the bulk bandgap is not even well-defined. More intriguingly, the number of trapped states equals the number of lattice sites along the normal direction of the boundary. We provide two configurations and validate the existence of this peculiar finite barrier-bound state experimentally in a dielectric photonic crystal at microwave frequencies. Our work offers extreme flexibility in tuning the coupling between localized states and channels as well as a new mechanism that facilitates unprecedented manipulation of light.
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Affiliation(s)
- Tao Liu
- Key Laboratory of Artificial Micro- and Nano-structures of Ministry of Education and School of Physics and Technology, Wuhan University, 430072, Wuhan, China
| | - Kai Bai
- Key Laboratory of Artificial Micro- and Nano-structures of Ministry of Education and School of Physics and Technology, Wuhan University, 430072, Wuhan, China
| | - Yicheng Zhang
- Key Laboratory of Artificial Micro- and Nano-structures of Ministry of Education and School of Physics and Technology, Wuhan University, 430072, Wuhan, China
| | - Duanduan Wan
- Key Laboratory of Artificial Micro- and Nano-structures of Ministry of Education and School of Physics and Technology, Wuhan University, 430072, Wuhan, China.
| | - Yun Lai
- National Laboratory of Solid State Microstructures, School of Physics, and Collaborative Innovation Center of Advanced Microstructures, Nanjing University, 210093, Nanjing, China
| | - C T Chan
- Department of Physics, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, 999077, Hong Kong, China
| | - Meng Xiao
- Key Laboratory of Artificial Micro- and Nano-structures of Ministry of Education and School of Physics and Technology, Wuhan University, 430072, Wuhan, China.
- Wuhan Institute of Quantum Technology, 430206, Wuhan, China.
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35
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Sun X, Suriyage M, Khan AR, Gao M, Zhao J, Liu B, Hasan MM, Rahman S, Chen RS, Lam PK, Lu Y. Twisted van der Waals Quantum Materials: Fundamentals, Tunability, and Applications. Chem Rev 2024; 124:1992-2079. [PMID: 38335114 DOI: 10.1021/acs.chemrev.3c00627] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 02/12/2024]
Abstract
Twisted van der Waals (vdW) quantum materials have emerged as a rapidly developing field of two-dimensional (2D) semiconductors. These materials establish a new central research area and provide a promising platform for studying quantum phenomena and investigating the engineering of novel optoelectronic properties such as single photon emission, nonlinear optical response, magnon physics, and topological superconductivity. These captivating electronic and optical properties result from, and can be tailored by, the interlayer coupling using moiré patterns formed by vertically stacking atomic layers with controlled angle misorientation or lattice mismatch. Their outstanding properties and the high degree of tunability position them as compelling building blocks for both compact quantum-enabled devices and classical optoelectronics. This paper offers a comprehensive review of recent advancements in the understanding and manipulation of twisted van der Waals structures and presents a survey of the state-of-the-art research on moiré superlattices, encompassing interdisciplinary interests. It delves into fundamental theories, synthesis and fabrication, and visualization techniques, and the wide range of novel physical phenomena exhibited by these structures, with a focus on their potential for practical device integration in applications ranging from quantum information to biosensors, and including classical optoelectronics such as modulators, light emitting diodes, lasers, and photodetectors. It highlights the unique ability of moiré superlattices to connect multiple disciplines, covering chemistry, electronics, optics, photonics, magnetism, topological and quantum physics. This comprehensive review provides a valuable resource for researchers interested in moiré superlattices, shedding light on their fundamental characteristics and their potential for transformative applications in various fields.
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Affiliation(s)
- Xueqian Sun
- School of Engineering, College of Engineering and Computer Science, The Australian National University, Canberra, Australian Capital Territory 2601, Australia
| | - Manuka Suriyage
- School of Engineering, College of Engineering and Computer Science, The Australian National University, Canberra, Australian Capital Territory 2601, Australia
| | - Ahmed Raza Khan
- School of Engineering, College of Engineering and Computer Science, The Australian National University, Canberra, Australian Capital Territory 2601, Australia
- Department of Industrial and Manufacturing Engineering, University of Engineering and Technology (Rachna College Campus), Gujranwala, Lahore 54700, Pakistan
| | - Mingyuan Gao
- School of Engineering, College of Engineering and Computer Science, The Australian National University, Canberra, Australian Capital Territory 2601, Australia
- College of Engineering and Technology, Southwest University, Chongqing 400716, China
| | - Jie Zhao
- Department of Quantum Science & Technology, Research School of Physics, The Australian National University, Canberra, Australian Capital Territory 2601, Australia
- Australian Research Council Centre of Excellence for Quantum Computation and Communication Technology, The Australian National University, Canberra, Australian Capital Territory 2601, Australia
| | - Boqing Liu
- School of Engineering, College of Engineering and Computer Science, The Australian National University, Canberra, Australian Capital Territory 2601, Australia
| | - Md Mehedi Hasan
- School of Engineering, College of Engineering and Computer Science, The Australian National University, Canberra, Australian Capital Territory 2601, Australia
| | - Sharidya Rahman
- Department of Materials Science and Engineering, Monash University, Clayton, Victoria 3800, Australia
- ARC Centre of Excellence in Exciton Science, Monash University, Clayton, Victoria 3800, Australia
| | - Ruo-Si Chen
- School of Engineering, College of Engineering and Computer Science, The Australian National University, Canberra, Australian Capital Territory 2601, Australia
| | - Ping Koy Lam
- Department of Quantum Science & Technology, Research School of Physics, The Australian National University, Canberra, Australian Capital Territory 2601, Australia
- Institute of Materials Research and Engineering (IMRE), Agency for Science, Technology and Research (A*STAR), 2 Fusionopolis Way, Innovis #08-03, Singapore 138634, Republic of Singapore
- Australian Research Council Centre of Excellence for Quantum Computation and Communication Technology, The Australian National University, Canberra, Australian Capital Territory 2601, Australia
| | - Yuerui Lu
- School of Engineering, College of Engineering and Computer Science, The Australian National University, Canberra, Australian Capital Territory 2601, Australia
- Australian Research Council Centre of Excellence for Quantum Computation and Communication Technology, The Australian National University, Canberra, Australian Capital Territory 2601, Australia
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Lomonte E, Stappers M, Krämer L, Pernice WHP, Lenzini F. Scalable and efficient grating couplers on low-index photonic platforms enabled by cryogenic deep silicon etching. Sci Rep 2024; 14:4256. [PMID: 38383577 PMCID: PMC10881461 DOI: 10.1038/s41598-024-53975-4] [Citation(s) in RCA: 4] [Impact Index Per Article: 4.0] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 06/29/2023] [Accepted: 02/07/2024] [Indexed: 02/23/2024] Open
Abstract
Efficient fiber-to-chip couplers for multi-port access to photonic integrated circuits are paramount for a broad class of applications, ranging, e.g., from telecommunication to photonic computing and quantum technologies. Grating-based approaches are often desirable for providing out-of-plane access to the photonic circuits. However, on photonic platforms characterized by a refractive index ≃ 2 at telecom wavelength, such as silicon nitride or thin-film lithium niobate, the limited scattering strength has thus far hindered the achievement of coupling efficiencies comparable to the ones attainable in silicon photonics. Here we present a flexible strategy for the realization of highly efficient grating couplers on such low-index photonic platforms. To simultaneously reach a high scattering efficiency and a near-unitary modal overlap with optical fibers, we make use of self-imaging gratings designed with a negative diffraction angle. To ensure high directionality of the diffracted light, we take advantage of a metal back-reflector patterned underneath the grating structure by cryogenic deep reactive ion etching of the silicon handle. Using silicon nitride as a testbed material, we experimentally demonstrate coupling efficiency up to - 0.55 dB in the telecom C-band with high chip-scale device yield.
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Affiliation(s)
- Emma Lomonte
- Institute of Physics, University of Münster, Wilhelm-Klemm-Straße 10, 48149, Münster, Germany
- CeNTech-Center for Nanotechnology, Heisenbergstraße 11, 48149, Münster, Germany
- SoN-Center for Soft Nanoscience, Busso-Peus-Straße 10, 48149, Münster, Germany
| | - Maik Stappers
- Institute of Physics, University of Münster, Wilhelm-Klemm-Straße 10, 48149, Münster, Germany
- CeNTech-Center for Nanotechnology, Heisenbergstraße 11, 48149, Münster, Germany
- SoN-Center for Soft Nanoscience, Busso-Peus-Straße 10, 48149, Münster, Germany
| | - Linus Krämer
- Institute of Physics, University of Münster, Wilhelm-Klemm-Straße 10, 48149, Münster, Germany
- CeNTech-Center for Nanotechnology, Heisenbergstraße 11, 48149, Münster, Germany
- SoN-Center for Soft Nanoscience, Busso-Peus-Straße 10, 48149, Münster, Germany
- Heidelberg University, Im Neuenheimer Feld 227, 69120, Heidelberg, Germany
| | - Wolfram H P Pernice
- Institute of Physics, University of Münster, Wilhelm-Klemm-Straße 10, 48149, Münster, Germany.
- CeNTech-Center for Nanotechnology, Heisenbergstraße 11, 48149, Münster, Germany.
- SoN-Center for Soft Nanoscience, Busso-Peus-Straße 10, 48149, Münster, Germany.
- Heidelberg University, Im Neuenheimer Feld 227, 69120, Heidelberg, Germany.
| | - Francesco Lenzini
- Institute of Physics, University of Münster, Wilhelm-Klemm-Straße 10, 48149, Münster, Germany.
- CeNTech-Center for Nanotechnology, Heisenbergstraße 11, 48149, Münster, Germany.
- SoN-Center for Soft Nanoscience, Busso-Peus-Straße 10, 48149, Münster, Germany.
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Li XK, Ma JX, Li XY, Hu JJ, Ding CY, Han FK, Guo XM, Tan X, Jin XM. High-efficiency reinforcement learning with hybrid architecture photonic integrated circuit. Nat Commun 2024; 15:1044. [PMID: 38316815 PMCID: PMC10844654 DOI: 10.1038/s41467-024-45305-z] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 06/09/2023] [Accepted: 01/18/2024] [Indexed: 02/07/2024] Open
Abstract
Reinforcement learning (RL) stands as one of the three fundamental paradigms within machine learning and has made a substantial leap to build general-purpose learning systems. However, using traditional electrical computers to simulate agent-environment interactions in RL models consumes tremendous computing resources, posing a significant challenge to the efficiency of RL. Here, we propose a universal framework that utilizes a photonic integrated circuit (PIC) to simulate the interactions in RL for improving the algorithm efficiency. High parallelism and precision on-chip optical interaction calculations are implemented with the assistance of link calibration in the hybrid architecture PIC. By introducing similarity information into the reward function of the RL model, PIC-RL successfully accomplishes perovskite materials synthesis task within a 3472-dimensional state space, resulting in a notable 56% improvement in efficiency. Our results validate the effectiveness of simulating RL algorithm interactions on the PIC platform, highlighting its potential to boost computing power in large-scale and sophisticated RL tasks.
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Affiliation(s)
- Xuan-Kun Li
- Center for Integrated Quantum Information Technologies (IQIT), School of Physics and Astronomy and State Key Laboratory of Advanced Optical Communication Systems and Networks, Shanghai Jiao Tong University, Shanghai, 200240, China
- Hefei National Laboratory, Hefei, 230088, China
| | - Jian-Xu Ma
- TuringQ Co., Ltd., Shanghai, 200240, China
| | | | - Jun-Jie Hu
- Center for Integrated Quantum Information Technologies (IQIT), School of Physics and Astronomy and State Key Laboratory of Advanced Optical Communication Systems and Networks, Shanghai Jiao Tong University, Shanghai, 200240, China
- Hefei National Laboratory, Hefei, 230088, China
| | - Chuan-Yang Ding
- Center for Integrated Quantum Information Technologies (IQIT), School of Physics and Astronomy and State Key Laboratory of Advanced Optical Communication Systems and Networks, Shanghai Jiao Tong University, Shanghai, 200240, China
- Hefei National Laboratory, Hefei, 230088, China
| | - Feng-Kai Han
- Center for Integrated Quantum Information Technologies (IQIT), School of Physics and Astronomy and State Key Laboratory of Advanced Optical Communication Systems and Networks, Shanghai Jiao Tong University, Shanghai, 200240, China
- Hefei National Laboratory, Hefei, 230088, China
| | | | - Xi Tan
- Center for Integrated Quantum Information Technologies (IQIT), School of Physics and Astronomy and State Key Laboratory of Advanced Optical Communication Systems and Networks, Shanghai Jiao Tong University, Shanghai, 200240, China
- Hefei National Laboratory, Hefei, 230088, China
| | - Xian-Min Jin
- Center for Integrated Quantum Information Technologies (IQIT), School of Physics and Astronomy and State Key Laboratory of Advanced Optical Communication Systems and Networks, Shanghai Jiao Tong University, Shanghai, 200240, China.
- Hefei National Laboratory, Hefei, 230088, China.
- TuringQ Co., Ltd., Shanghai, 200240, China.
- Chip Hub for Integrated Photonics Xplore (CHIPX), Shanghai Jiao Tong University, Wuxi, 214000, China.
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38
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Shang K, Niu L, Jin H, Wang H, Zhang W, Gan F, Xu P. Non-volatile 2 × 2 optical switch using multimode interference in an Sb 2Se 3-loaded waveguide. OPTICS LETTERS 2024; 49:722-725. [PMID: 38300099 DOI: 10.1364/ol.511301] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/07/2023] [Accepted: 12/18/2023] [Indexed: 02/02/2024]
Abstract
We propose a non-volatile 2 × 2 photonic switch based on multimode interference in an Sb2Se3-loaded waveguide. The different modal symmetries of the TE0 and TE1 modes supported in the multimode region change their propagation constants distinctly upon the Sb2Se3 phase transition. Through careful optical design and FDTD optimization of the multimode waveguide dimensions, efficient switching is achieved despite the modest index contrast of Sb2Se3 relative to Ge2Sb2Te5. The fabricated optical switch demonstrates favorable characteristics, including low insertion loss of ∼1 dB, a compact length of ∼27 µm, and small cross talk below -15 dB across a 35 nm bandwidth. Such non-volatile and broadband components will be critical for future high-density programmable photonic-integrated circuits for optical communications and signal processing.
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Fang Z, Mills B, Chen R, Zhang J, Xu P, Hu J, Majumdar A. Arbitrary Programming of Racetrack Resonators Using Low-Loss Phase-Change Material Sb 2Se 3. NANO LETTERS 2024; 24:97-103. [PMID: 38127716 DOI: 10.1021/acs.nanolett.3c03353] [Citation(s) in RCA: 3] [Impact Index Per Article: 3.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 12/23/2023]
Abstract
The programmable photonic integrated circuit (PIC) is an enabling technology behind optical interconnects and quantum information processing. Conventionally, the programmability of PICs is driven by the thermo-optic effect, free carrier dispersion, or mechanical tuning. These effects afford either high speed or a large extinction ratio, but all require constant power or bias to maintain the states, which is undesirable for programmability with infrequent switching. Recent progress in programmable PICs based on nonvolatile phase-change materials (PCMs) offers an attractive solution to a truly "set-and-forget" switch that requires zero static energy. Here, we report an essential building block of large-scale programmable PICs─a racetrack resonator with independent control of coupling and phase. We changed the resonance extinction ratio (ER) without perturbing the resonance wavelength, leveraging a programmable unit based on a directional coupler and a low-loss PCM Sb2Se3. The unit is only 33-μm-long and has an operating bandwidth over 50 nm, a low insertion loss (∼0.36 dB), high ER (∼15 dB), and excellent fabrication yield of over 1000 cycles endurance across nine switches. The work is a crucial step toward future large-scale energy-efficient programmable PICs.
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Affiliation(s)
- Zhuoran Fang
- Department of Electrical and Computer Engineering, University of Washington, Seattle, Washington 98195, United States
| | - Brian Mills
- Department of Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, United States
| | - Rui Chen
- Department of Electrical and Computer Engineering, University of Washington, Seattle, Washington 98195, United States
| | - Jieying Zhang
- Faculty of Electrical Engineering and Computer Science, Ningbo University, Ningbo 315211, China
- Key Laboratory of Photoelectric Detection Materials and Devices of Zhejiang Province, Ningbo 315211, China
| | - Peipeng Xu
- Faculty of Electrical Engineering and Computer Science, Ningbo University, Ningbo 315211, China
- Key Laboratory of Photoelectric Detection Materials and Devices of Zhejiang Province, Ningbo 315211, China
| | - Juejun Hu
- Department of Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, United States
| | - Arka Majumdar
- Department of Electrical and Computer Engineering, University of Washington, Seattle, Washington 98195, United States
- Department of Physics, University of Washington, Seattle, Washington 98195, United States
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40
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Bonde B, Patil P, Choubey B. The Future of Drug Development with Quantum Computing. Methods Mol Biol 2024; 2716:153-179. [PMID: 37702939 DOI: 10.1007/978-1-0716-3449-3_7] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 09/14/2023]
Abstract
Novel medication development is a time-consuming and expensive multistage procedure. Recent technology developments have lowered timeframes, complexity, and cost dramatically. Current research projects are driven by AI and machine learning computational models. This chapter will introduce quantum computing (QC) to drug development issues and provide an in-depth discussion of how quantum computing may be used to solve various drug discovery problems. We will first discuss the fundamentals of QC, a review of known Hamiltonians, how to apply Hamiltonians to drug discovery challenges, and what the noisy intermediate-scale quantum (NISQ) era methods and their limitations are.We will further discuss how these NISQ era techniques can aid with specific drug discovery challenges, including protein folding, molecular docking, AI-/ML-based optimization, and novel modalities for small molecules and RNA secondary structures. Consequently, we will discuss the latest QC landscape's opportunities and challenges.
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Affiliation(s)
- Bhushan Bonde
- Evotec (UK) Ltd., Oxfordshire, UK.
- Digital Futures Institute, University of Suffolk, Ipswich, UK.
| | - Pratik Patil
- Evotec (UK) Ltd., Oxfordshire, UK
- Digital Futures Institute, University of Suffolk, Ipswich, UK
| | - Bhaskar Choubey
- Digital Futures Institute, University of Suffolk, Ipswich, UK
- Chair of Analogue Circuits and Image Sensors, Siegen University, Siegen, Germany
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41
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Tokman M, Verma JK, Bohreer J, Belyanin A. Maximally Efficient Biphoton Generation by Single Photon Decay in Nonlinear Quantum Photonic Circuits. PHYSICAL REVIEW LETTERS 2023; 131:233802. [PMID: 38134774 DOI: 10.1103/physrevlett.131.233802] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/05/2023] [Accepted: 11/07/2023] [Indexed: 12/24/2023]
Abstract
We develop a general nonperturbative formalism and propose a specific scheme for maximally efficient generation of biphoton states by parametric decay of single photons. We show that the well-known critical coupling concept of integrated optics can be generalized to the nonlinear coupling of quantized photon modes to describe the nonperturbative optimal regime of a single-photon nonlinearity and establish a fundamental upper limit on the nonlinear generation efficiency of quantum-correlated photons, which approaches unity for low enough absorption losses.
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Affiliation(s)
- Mikhail Tokman
- Department of Electrical and Electronic Engineering and Schlesinger Knowledge Center for Compact Accelerators and Radiation Sources, Ariel University, 40700 Ariel, Israel
| | - Jitendra K Verma
- Department of Physics and Astronomy, Texas A&M University, College Station, Texas 77843 USA
| | - Jacob Bohreer
- Department of Physics and Astronomy, Texas A&M University, College Station, Texas 77843 USA
| | - Alexey Belyanin
- Department of Physics and Astronomy, Texas A&M University, College Station, Texas 77843 USA
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42
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Clementi M, Nitiss E, Liu J, Durán-Valdeiglesias E, Belahsene S, Debrégeas H, Kippenberg TJ, Brès CS. A chip-scale second-harmonic source via self-injection-locked all-optical poling. LIGHT, SCIENCE & APPLICATIONS 2023; 12:296. [PMID: 38062066 PMCID: PMC10703906 DOI: 10.1038/s41377-023-01329-6] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 07/24/2023] [Revised: 10/10/2023] [Accepted: 11/06/2023] [Indexed: 03/27/2024]
Abstract
Second-harmonic generation allows for coherently bridging distant regions of the optical spectrum, with applications ranging from laser technology to self-referencing of frequency combs. However, accessing the nonlinear response of a medium typically requires high-power bulk sources, specific nonlinear crystals, and complex optical setups, hindering the path toward large-scale integration. Here we address all of these issues by engineering a chip-scale second-harmonic (SH) source based on the frequency doubling of a semiconductor laser self-injection-locked to a silicon nitride microresonator. The injection-locking mechanism, combined with a high-Q microresonator, results in an ultra-narrow intrinsic linewidth at the fundamental harmonic frequency as small as 41 Hz. Owing to the extreme resonant field enhancement, quasi-phase-matched second-order nonlinearity is photoinduced through the coherent photogalvanic effect and the high coherence is mapped on the generated SH field. We show how such optical poling technique can be engineered to provide efficient SH generation across the whole C and L telecom bands, in a reconfigurable fashion, overcoming the need for poling electrodes. Our device operates with milliwatt-level pumping and outputs SH power exceeding 2 mW, for an efficiency as high as 280%/W under electrical driving. Our findings suggest that standalone, highly-coherent, and efficient SH sources can be integrated in current silicon nitride photonics, unlocking the potential of χ(2) processes in the next generation of integrated photonic devices.
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Affiliation(s)
- Marco Clementi
- Photonic Systems Laboratory (PHOSL), École Polytechnique Fédérale de Lausanne, 1015, Lausanne, Switzerland.
| | - Edgars Nitiss
- Photonic Systems Laboratory (PHOSL), École Polytechnique Fédérale de Lausanne, 1015, Lausanne, Switzerland
| | - Junqiu Liu
- Laboratory of Photonics and Quantum Measurements (LPQM), École Polytechnique Fédérale de Lausanne, 1015, Lausanne, Switzerland
| | | | | | | | - Tobias J Kippenberg
- Laboratory of Photonics and Quantum Measurements (LPQM), École Polytechnique Fédérale de Lausanne, 1015, Lausanne, Switzerland
| | - Camille-Sophie Brès
- Photonic Systems Laboratory (PHOSL), École Polytechnique Fédérale de Lausanne, 1015, Lausanne, Switzerland.
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43
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Prabhathan P, Sreekanth KV, Teng J, Ko JH, Yoo YJ, Jeong HH, Lee Y, Zhang S, Cao T, Popescu CC, Mills B, Gu T, Fang Z, Chen R, Tong H, Wang Y, He Q, Lu Y, Liu Z, Yu H, Mandal A, Cui Y, Ansari AS, Bhingardive V, Kang M, Lai CK, Merklein M, Müller MJ, Song YM, Tian Z, Hu J, Losurdo M, Majumdar A, Miao X, Chen X, Gholipour B, Richardson KA, Eggleton BJ, Sharda K, Wuttig M, Singh R. Roadmap for phase change materials in photonics and beyond. iScience 2023; 26:107946. [PMID: 37854690 PMCID: PMC10579438 DOI: 10.1016/j.isci.2023.107946] [Citation(s) in RCA: 16] [Impact Index Per Article: 8.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 10/20/2023] Open
Abstract
Phase Change Materials (PCMs) have demonstrated tremendous potential as a platform for achieving diverse functionalities in active and reconfigurable micro-nanophotonic devices across the electromagnetic spectrum, ranging from terahertz to visible frequencies. This comprehensive roadmap reviews the material and device aspects of PCMs, and their diverse applications in active and reconfigurable micro-nanophotonic devices across the electromagnetic spectrum. It discusses various device configurations and optimization techniques, including deep learning-based metasurface design. The integration of PCMs with Photonic Integrated Circuits and advanced electric-driven PCMs are explored. PCMs hold great promise for multifunctional device development, including applications in non-volatile memory, optical data storage, photonics, energy harvesting, biomedical technology, neuromorphic computing, thermal management, and flexible electronics.
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Affiliation(s)
- Patinharekandy Prabhathan
- Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University, 21 Nanyang Link, Singapore 637371, Singapore
- Centre for Disruptive Photonic Technologies, The Photonic Institute, 50 Nanyang Avenue, Singapore 639798, Singapore
| | - Kandammathe Valiyaveedu Sreekanth
- Institute of Materials Research and Engineering (IMRE), Agency for Science, Technology and Research (A∗STAR), 2 Fusionopolis Way, Innovis #08-03, Singapore 138634, Republic of Singapore
| | - Jinghua Teng
- Institute of Materials Research and Engineering (IMRE), Agency for Science, Technology and Research (A∗STAR), 2 Fusionopolis Way, Innovis #08-03, Singapore 138634, Republic of Singapore
| | - Joo Hwan Ko
- School of Electrical Engineering and Computer Science, Gwangju Institute of Science and Technology, Gwangju 61005, Republic of Korea
| | - Young Jin Yoo
- School of Electrical Engineering and Computer Science, Gwangju Institute of Science and Technology, Gwangju 61005, Republic of Korea
| | - Hyeon-Ho Jeong
- School of Electrical Engineering and Computer Science, Gwangju Institute of Science and Technology, Gwangju 61005, Republic of Korea
| | - Yubin Lee
- School of Materials Science and Engineering, Gwangju Institute of Science and Technology, Gwangju 61005, Republic of Korea
| | - Shoujun Zhang
- DELL, Center for Terahertz Waves and College of Precision Instrument and Optoelectronics Engineering, Key Laboratory of Optoelectronic Information Technology (Ministry of Education of China), Tianjin University, Tianjin 300072, China
| | - Tun Cao
- DELL, School of Optoelectronic Engineering and Instrumentation Science, Dalian University of Technology, Dalian 116024, China
| | - Cosmin-Constantin Popescu
- Department of Materials Science & Engineering, Massachusetts Institute of Technology, Cambridge, MA, USA
| | - Brian Mills
- Department of Materials Science & Engineering, Massachusetts Institute of Technology, Cambridge, MA, USA
| | - Tian Gu
- Department of Materials Science & Engineering, Massachusetts Institute of Technology, Cambridge, MA, USA
- Materials Research Laboratory, Massachusetts Institute of Technology, Cambridge, MA, USA
| | - Zhuoran Fang
- Department of Electrical & Computer Engineering, University of Washington, Washington, Seattle, USA
| | - Rui Chen
- Department of Electrical & Computer Engineering, University of Washington, Washington, Seattle, USA
| | - Hao Tong
- Wuhan National Research Center for Optoelectronics, School of Optical and Electronic Information, Huazhong University of Science and Technology, Wuhan, China
| | - Yi Wang
- Wuhan National Research Center for Optoelectronics, School of Optical and Electronic Information, Huazhong University of Science and Technology, Wuhan, China
| | - Qiang He
- Wuhan National Research Center for Optoelectronics, School of Optical and Electronic Information, Huazhong University of Science and Technology, Wuhan, China
| | - Yitao Lu
- Wuhan National Research Center for Optoelectronics, School of Optical and Electronic Information, Huazhong University of Science and Technology, Wuhan, China
| | - Zhiyuan Liu
- Wuhan National Research Center for Optoelectronics, School of Optical and Electronic Information, Huazhong University of Science and Technology, Wuhan, China
| | - Han Yu
- Institute of Advanced Materials, Beijing Normal University, Beijing 100875, China
| | - Avik Mandal
- Nanoscale Optics Lab, ECE Department, University of Alberta, Edmonton, Canada
| | - Yihao Cui
- Nanoscale Optics Lab, ECE Department, University of Alberta, Edmonton, Canada
| | - Abbas Sheikh Ansari
- Nanoscale Optics Lab, ECE Department, University of Alberta, Edmonton, Canada
| | - Viraj Bhingardive
- Nanoscale Optics Lab, ECE Department, University of Alberta, Edmonton, Canada
| | - Myungkoo Kang
- CREOL, College of Optics and Photonics, University of Central Florida, Orlando, FL, USA
| | - Choon Kong Lai
- Institute of Photonics and Optical Science (IPOS), School of Physics, The University of Sydney, New South Wales, NSW 2006, Australia
- The University of Sydney Nano Institute (Sydney Nano), The University of Sydney, New South Wales, NSW 2006, Australia
| | - Moritz Merklein
- Institute of Photonics and Optical Science (IPOS), School of Physics, The University of Sydney, New South Wales, NSW 2006, Australia
- The University of Sydney Nano Institute (Sydney Nano), The University of Sydney, New South Wales, NSW 2006, Australia
| | | | - Young Min Song
- School of Electrical Engineering and Computer Science, Gwangju Institute of Science and Technology, Gwangju 61005, Republic of Korea
- Anti-Viral Research Center, Gwangju Institute of Science and Technology, Gwangju 61005, Republic of Korea
- AI Graduate School, Gwangju Institute of Science and Technology, Gwangju 61005, Republic of Korea
| | - Zhen Tian
- DELL, Center for Terahertz Waves and College of Precision Instrument and Optoelectronics Engineering, Key Laboratory of Optoelectronic Information Technology (Ministry of Education of China), Tianjin University, Tianjin 300072, China
| | - Juejun Hu
- Department of Materials Science & Engineering, Massachusetts Institute of Technology, Cambridge, MA, USA
- Materials Research Laboratory, Massachusetts Institute of Technology, Cambridge, MA, USA
| | - Maria Losurdo
- Istituto di Chimica della Materia Condensata e di Tecnologie per l'Energia, CNR-ICMATE, Corso Stati Uniti 4, 35127 Padova, Italy
| | - Arka Majumdar
- Department of Electrical & Computer Engineering, University of Washington, Washington, Seattle, USA
| | - Xiangshui Miao
- Wuhan National Research Center for Optoelectronics, School of Optical and Electronic Information, Huazhong University of Science and Technology, Wuhan, China
| | - Xiao Chen
- Institute of Advanced Materials, Beijing Normal University, Beijing 100875, China
| | - Behrad Gholipour
- Nanoscale Optics Lab, ECE Department, University of Alberta, Edmonton, Canada
| | - Kathleen A. Richardson
- CREOL, College of Optics and Photonics, University of Central Florida, Orlando, FL, USA
- Department of Materials Science and Engineering, University of Central Florida, Orlando, FL, USA
| | - Benjamin J. Eggleton
- Institute of Photonics and Optical Science (IPOS), School of Physics, The University of Sydney, New South Wales, NSW 2006, Australia
- The University of Sydney Nano Institute (Sydney Nano), The University of Sydney, New South Wales, NSW 2006, Australia
| | - Kanudha Sharda
- iScience, Cell Press, 125 London Wall, Barbican, London EC2Y 5AJ, UK
- iScience, Cell Press, RELX India Pvt Ltd., 14th Floor, Building No. 10B, DLF Cyber City, Phase II, Gurugram, Haryana 122002, India
| | - Matthias Wuttig
- Institute of Physics IA, RWTH Aachen University, 52074 Aachen, Germany
- Peter Grünberg Institute (PGI 10), Forschungszentrum Jülich, 52428 Jülich, Germany
| | - Ranjan Singh
- Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University, 21 Nanyang Link, Singapore 637371, Singapore
- Centre for Disruptive Photonic Technologies, The Photonic Institute, 50 Nanyang Avenue, Singapore 639798, Singapore
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44
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He XL, Lu Y, Bao DQ, Xue H, Jiang WB, Wang Z, Roudsari AF, Delsing P, Tsai JS, Lin ZR. Fast generation of Schrödinger cat states using a Kerr-tunable superconducting resonator. Nat Commun 2023; 14:6358. [PMID: 37821443 PMCID: PMC10567735 DOI: 10.1038/s41467-023-42057-0] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 04/06/2023] [Accepted: 09/28/2023] [Indexed: 10/13/2023] Open
Abstract
Schrödinger cat states, quantum superpositions of macroscopically distinct classical states, are an important resource for quantum communication, quantum metrology and quantum computation. Especially, cat states in a phase space protected against phase-flip errors can be used as a logical qubit. However, cat states, normally generated in three-dimensional cavities and/or strong multi-photon drives, are facing the challenges of scalability and controllability. Here, we present a strategy to generate and preserve cat states in a coplanar superconducting circuit by the fast modulation of Kerr nonlinearity. At the Kerr-free work point, our cat states are passively preserved due to the vanishing Kerr effect. We are able to prepare a 2-component cat state in our chip-based device with a fidelity reaching 89.1% under a 96 ns gate time. Our scheme shows an excellent route to constructing a chip-based bosonic quantum processor.
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Affiliation(s)
- X L He
- National Key Laboratory of Materials for Integrated Circuits, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, 200050, Shanghai, China
- University of Chinese Academy of Science, 100049, Beijing, China
| | - Yong Lu
- 3rd Physikalisches Institut, University of Stuttgart, 70569, Stuttgart, Germany.
- Microtechnology and Nanoscience, Chalmers University of Technology, SE-412 96, Göteborg, Sweden.
| | - D Q Bao
- National Key Laboratory of Materials for Integrated Circuits, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, 200050, Shanghai, China
- University of Chinese Academy of Science, 100049, Beijing, China
| | - Hang Xue
- National Key Laboratory of Materials for Integrated Circuits, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, 200050, Shanghai, China
- University of Chinese Academy of Science, 100049, Beijing, China
| | - W B Jiang
- National Key Laboratory of Materials for Integrated Circuits, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, 200050, Shanghai, China
- University of Chinese Academy of Science, 100049, Beijing, China
| | - Z Wang
- National Key Laboratory of Materials for Integrated Circuits, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, 200050, Shanghai, China
- University of Chinese Academy of Science, 100049, Beijing, China
| | - A F Roudsari
- Microtechnology and Nanoscience, Chalmers University of Technology, SE-412 96, Göteborg, Sweden
| | - Per Delsing
- Microtechnology and Nanoscience, Chalmers University of Technology, SE-412 96, Göteborg, Sweden
| | - J S Tsai
- Graduate School of Science, Tokyo University of Science, Shinjuku, Tokyo, 162-0825, Japan
- Center for Quantum Computing, RIKEN, Wako, Saitama, 351-0198, Japan
| | - Z R Lin
- National Key Laboratory of Materials for Integrated Circuits, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, 200050, Shanghai, China.
- University of Chinese Academy of Science, 100049, Beijing, China.
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45
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Stefszky M, Vom Bruch F, Santandrea M, Ricken R, Quiring V, Eigner C, Herrmann H, Silberhorn C. Lithium niobate waveguide squeezer with integrated cavity length stabilisation for network applications. OPTICS EXPRESS 2023; 31:34903-34916. [PMID: 37859235 DOI: 10.1364/oe.498423] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/21/2023] [Accepted: 08/24/2023] [Indexed: 10/21/2023]
Abstract
We report a titanium indiffused waveguide resonator featuring an integrated electro-optic modulator for cavity length stabilisation that produces close to 5 dB of squeezed light at 1550 nm (2.4 dB directly measured). The resonator is locked on resonance for tens of minutes with 70 mW of SH light incident on the cavity, demonstrating that photorefraction can be mitigated. Squeezed light production concurrent with cavity length stabilisation utilising the integrated EOM is demonstrated. The device demonstrates the suitability of this platform for squeezed light generation in network applications, where stabilisation to the reference field is typically necessary.
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46
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Yu S, Zhong ZP, Fang Y, Patel RB, Li QP, Liu W, Li Z, Xu L, Sagona-Stophel S, Mer E, Thomas SE, Meng Y, Li ZP, Yang YZ, Wang ZA, Guo NJ, Zhang WH, Tranmer GK, Dong Y, Wang YT, Tang JS, Li CF, Walmsley IA, Guo GC. A universal programmable Gaussian boson sampler for drug discovery. NATURE COMPUTATIONAL SCIENCE 2023; 3:839-848. [PMID: 38177757 PMCID: PMC10768638 DOI: 10.1038/s43588-023-00526-y] [Citation(s) in RCA: 7] [Impact Index Per Article: 3.5] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Grants] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 12/16/2022] [Accepted: 09/01/2023] [Indexed: 01/06/2024]
Abstract
Gaussian boson sampling (GBS) has the potential to solve complex graph problems, such as clique finding, which is relevant to drug discovery tasks. However, realizing the full benefits of quantum enhancements requires large-scale quantum hardware with universal programmability. Here we have developed a time-bin-encoded GBS photonic quantum processor that is universal, programmable and software-scalable. Our processor features freely adjustable squeezing parameters and can implement arbitrary unitary operations with a programmable interferometer. Leveraging our processor, we successfully executed clique finding on a 32-node graph, achieving approximately twice the success probability compared to classical sampling. As proof of concept, we implemented a versatile quantum drug discovery platform using this GBS processor, enabling molecular docking and RNA-folding prediction tasks. Our work achieves GBS circuitry with its universal and programmable architecture, advancing GBS toward use in real-world applications.
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Affiliation(s)
- Shang Yu
- Research Center for Quantum Sensing, Zhejiang Lab, Hangzhou, People's Republic of China.
- Quantum Optics and Laser Science, Blackett Laboratory, Imperial College London, London, UK.
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, China.
- CAS Center For Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, China.
| | - Zhi-Peng Zhong
- Research Center for Quantum Sensing, Zhejiang Lab, Hangzhou, People's Republic of China
| | - Yuhua Fang
- College of Pharmacy, Rady Faculty of Health Sciences, University of Manitoba, Winnipeg, Manitoba, Canada
| | - Raj B Patel
- Quantum Optics and Laser Science, Blackett Laboratory, Imperial College London, London, UK.
| | - Qing-Peng Li
- Research Center for Quantum Sensing, Zhejiang Lab, Hangzhou, People's Republic of China
| | - Wei Liu
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, China
- CAS Center For Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, China
| | - Zhenghao Li
- Quantum Optics and Laser Science, Blackett Laboratory, Imperial College London, London, UK
| | - Liang Xu
- Research Center for Quantum Sensing, Zhejiang Lab, Hangzhou, People's Republic of China
| | - Steven Sagona-Stophel
- Quantum Optics and Laser Science, Blackett Laboratory, Imperial College London, London, UK
| | - Ewan Mer
- Quantum Optics and Laser Science, Blackett Laboratory, Imperial College London, London, UK
| | - Sarah E Thomas
- Quantum Optics and Laser Science, Blackett Laboratory, Imperial College London, London, UK
| | - Yu Meng
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, China
- CAS Center For Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, China
| | - Zhi-Peng Li
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, China
- CAS Center For Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, China
| | - Yuan-Ze Yang
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, China
- CAS Center For Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, China
| | - Zhao-An Wang
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, China
- CAS Center For Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, China
| | - Nai-Jie Guo
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, China
- CAS Center For Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, China
| | - Wen-Hao Zhang
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, China
- CAS Center For Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, China
| | - Geoffrey K Tranmer
- College of Pharmacy, Rady Faculty of Health Sciences, University of Manitoba, Winnipeg, Manitoba, Canada
| | - Ying Dong
- Research Center for Quantum Sensing, Zhejiang Lab, Hangzhou, People's Republic of China
| | - Yi-Tao Wang
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, China.
- CAS Center For Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, China.
| | - Jian-Shun Tang
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, China.
- CAS Center For Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, China.
- Hefei National Laboratory, University of Science and Technology of China, Hefei, China.
| | - Chuan-Feng Li
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, China.
- CAS Center For Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, China.
- Hefei National Laboratory, University of Science and Technology of China, Hefei, China.
| | - Ian A Walmsley
- Quantum Optics and Laser Science, Blackett Laboratory, Imperial College London, London, UK
| | - Guang-Can Guo
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, China
- CAS Center For Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, China
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47
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Oripov BG, Rampini DS, Allmaras J, Shaw MD, Nam SW, Korzh B, McCaughan AN. A superconducting nanowire single-photon camera with 400,000 pixels. Nature 2023; 622:730-734. [PMID: 37880435 DOI: 10.1038/s41586-023-06550-2] [Citation(s) in RCA: 12] [Impact Index Per Article: 6.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 05/29/2023] [Accepted: 08/17/2023] [Indexed: 10/27/2023]
Abstract
For the past 50 years, superconducting detectors have offered exceptional sensitivity and speed for detecting faint electromagnetic signals in a wide range of applications. These detectors operate at very low temperatures and generate a minimum of excess noise, making them ideal for testing the non-local nature of reality1,2, investigating dark matter3,4, mapping the early universe5-7 and performing quantum computation8-10 and communication11-14. Despite their appealing properties, however, there are at present no large-scale superconducting cameras-even the largest demonstrations have never exceeded 20,000 pixels15. This is especially true for superconducting nanowire single-photon detectors (SNSPDs)16-18. These detectors have been demonstrated with system detection efficiencies of 98.0% (ref. 19), sub-3-ps timing jitter20, sensitivity from the ultraviolet21 to the mid-infrared22 and microhertz dark-count rates3, but have never achieved an array size larger than a kilopixel23,24. Here we report on the development of a 400,000-pixel SNSPD camera, a factor of 400 improvement over the state of the art. The array spanned an area of 4 × 2.5 mm with 5 × 5-μm resolution, reached unity quantum efficiency at wavelengths of 370 nm and 635 nm, counted at a rate of 1.1 × 105 counts per second (cps) and had a dark-count rate of 1.0 × 10-4 cps per detector (corresponding to 0.13 cps over the whole array). The imaging area contains no ancillary circuitry and the architecture is scalable well beyond the present demonstration, paving the way for large-format superconducting cameras with near-unity detection efficiencies across a wide range of the electromagnetic spectrum.
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Affiliation(s)
- B G Oripov
- National Institute of Standards and Technology, Boulder, CO, USA.
- Department of Physics, University of Colorado Boulder, Boulder, CO, USA.
| | - D S Rampini
- National Institute of Standards and Technology, Boulder, CO, USA
- Department of Physics, University of Colorado Boulder, Boulder, CO, USA
| | - J Allmaras
- Jet Propulsion Laboratory, California Institute of Technology, Pasadena, CA, USA
| | - M D Shaw
- Jet Propulsion Laboratory, California Institute of Technology, Pasadena, CA, USA
| | - S W Nam
- National Institute of Standards and Technology, Boulder, CO, USA
| | - B Korzh
- Jet Propulsion Laboratory, California Institute of Technology, Pasadena, CA, USA
| | - A N McCaughan
- National Institute of Standards and Technology, Boulder, CO, USA
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48
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Fu Z, Bao J, Wang J. Programmability empowering quantum boson sampling. NATURE COMPUTATIONAL SCIENCE 2023; 3:819-820. [PMID: 38177759 DOI: 10.1038/s43588-023-00534-y] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 01/06/2024]
Affiliation(s)
- Zhaorong Fu
- State Key Laboratory for Mesoscopic Physics, School of Physics, Peking University, Beijing, China
| | - Jueming Bao
- State Key Laboratory for Mesoscopic Physics, School of Physics, Peking University, Beijing, China
| | - Jianwei Wang
- State Key Laboratory for Mesoscopic Physics, School of Physics, Peking University, Beijing, China.
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49
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Li Z, Wang RN, Lihachev G, Zhang J, Tan Z, Churaev M, Kuznetsov N, Siddharth A, Bereyhi MJ, Riemensberger J, Kippenberg TJ. High density lithium niobate photonic integrated circuits. Nat Commun 2023; 14:4856. [PMID: 37563149 PMCID: PMC10415301 DOI: 10.1038/s41467-023-40502-8] [Citation(s) in RCA: 19] [Impact Index Per Article: 9.5] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 12/18/2022] [Accepted: 07/26/2023] [Indexed: 08/12/2023] Open
Abstract
Photonic integrated circuits have the potential to pervade into multiple applications traditionally limited to bulk optics. Of particular interest for new applications are ferroelectrics such as Lithium Niobate, which exhibit a large Pockels effect, but are difficult to process via dry etching. Here we demonstrate that diamond-like carbon (DLC) is a superior material for the manufacturing of photonic integrated circuits based on ferroelectrics, specifically LiNbO3. Using DLC as a hard mask, we demonstrate the fabrication of deeply etched, tightly confining, low loss waveguides with losses as low as 4 dB/m. In contrast to widely employed ridge waveguides, this approach benefits from a more than one order of magnitude higher area integration density while maintaining efficient electro-optical modulation, low loss, and offering a route for efficient optical fiber interfaces. As a proof of concept, we demonstrate a III-V/LiNbO3 based laser with sub-kHz intrinsic linewidth and tuning rate of 0.7 PHz/s with excellent linearity and CMOS-compatible driving voltage. We also demonstrated a MZM modulator with a 1.73 cm length and a halfwave voltage of 1.94 V.
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Affiliation(s)
- Zihan Li
- Institute of Physics, Swiss Federal Institute of Technology Lausanne (EPFL), CH-1015, Lausanne, Switzerland
- Center of Quantum Science and Engineering (EPFL), CH-1015, Lausanne, Switzerland
| | - Rui Ning Wang
- Institute of Physics, Swiss Federal Institute of Technology Lausanne (EPFL), CH-1015, Lausanne, Switzerland
- Center of Quantum Science and Engineering (EPFL), CH-1015, Lausanne, Switzerland
| | - Grigory Lihachev
- Institute of Physics, Swiss Federal Institute of Technology Lausanne (EPFL), CH-1015, Lausanne, Switzerland
- Center of Quantum Science and Engineering (EPFL), CH-1015, Lausanne, Switzerland
| | - Junyin Zhang
- Institute of Physics, Swiss Federal Institute of Technology Lausanne (EPFL), CH-1015, Lausanne, Switzerland
- Center of Quantum Science and Engineering (EPFL), CH-1015, Lausanne, Switzerland
| | - Zelin Tan
- Institute of Physics, Swiss Federal Institute of Technology Lausanne (EPFL), CH-1015, Lausanne, Switzerland
- Center of Quantum Science and Engineering (EPFL), CH-1015, Lausanne, Switzerland
| | - Mikhail Churaev
- Institute of Physics, Swiss Federal Institute of Technology Lausanne (EPFL), CH-1015, Lausanne, Switzerland
- Center of Quantum Science and Engineering (EPFL), CH-1015, Lausanne, Switzerland
| | - Nikolai Kuznetsov
- Institute of Physics, Swiss Federal Institute of Technology Lausanne (EPFL), CH-1015, Lausanne, Switzerland
- Center of Quantum Science and Engineering (EPFL), CH-1015, Lausanne, Switzerland
| | - Anat Siddharth
- Institute of Physics, Swiss Federal Institute of Technology Lausanne (EPFL), CH-1015, Lausanne, Switzerland
- Center of Quantum Science and Engineering (EPFL), CH-1015, Lausanne, Switzerland
| | - Mohammad J Bereyhi
- Institute of Physics, Swiss Federal Institute of Technology Lausanne (EPFL), CH-1015, Lausanne, Switzerland
- Center of Quantum Science and Engineering (EPFL), CH-1015, Lausanne, Switzerland
- Luxtelligence SA, CH-1015, Lausanne, Switzerland
| | - Johann Riemensberger
- Institute of Physics, Swiss Federal Institute of Technology Lausanne (EPFL), CH-1015, Lausanne, Switzerland
- Center of Quantum Science and Engineering (EPFL), CH-1015, Lausanne, Switzerland
| | - Tobias J Kippenberg
- Institute of Physics, Swiss Federal Institute of Technology Lausanne (EPFL), CH-1015, Lausanne, Switzerland.
- Center of Quantum Science and Engineering (EPFL), CH-1015, Lausanne, Switzerland.
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50
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Luo W, Cao L, Shi Y, Wan L, Zhang H, Li S, Chen G, Li Y, Li S, Wang Y, Sun S, Karim MF, Cai H, Kwek LC, Liu AQ. Recent progress in quantum photonic chips for quantum communication and internet. LIGHT, SCIENCE & APPLICATIONS 2023; 12:175. [PMID: 37443095 DOI: 10.1038/s41377-023-01173-8] [Citation(s) in RCA: 18] [Impact Index Per Article: 9.0] [Reference Citation Analysis] [Abstract] [Grants] [Subscribe] [Scholar Register] [Received: 08/07/2022] [Revised: 04/27/2023] [Accepted: 04/28/2023] [Indexed: 07/15/2023]
Abstract
Recent years have witnessed significant progress in quantum communication and quantum internet with the emerging quantum photonic chips, whose characteristics of scalability, stability, and low cost, flourish and open up new possibilities in miniaturized footprints. Here, we provide an overview of the advances in quantum photonic chips for quantum communication, beginning with a summary of the prevalent photonic integrated fabrication platforms and key components for integrated quantum communication systems. We then discuss a range of quantum communication applications, such as quantum key distribution and quantum teleportation. Finally, the review culminates with a perspective on challenges towards high-performance chip-based quantum communication, as well as a glimpse into future opportunities for integrated quantum networks.
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Affiliation(s)
- Wei Luo
- Quantum Science and Engineering Centre (QSec), Nanyang Technological University, Singapore, 639798, Singapore
| | - Lin Cao
- Quantum Science and Engineering Centre (QSec), Nanyang Technological University, Singapore, 639798, Singapore
| | - Yuzhi Shi
- Institute of Precision Optical Engineering, School of Physics Science and Engineering, Tongji University, 200092, Shanghai, China.
| | - Lingxiao Wan
- Quantum Science and Engineering Centre (QSec), Nanyang Technological University, Singapore, 639798, Singapore
| | - Hui Zhang
- Quantum Science and Engineering Centre (QSec), Nanyang Technological University, Singapore, 639798, Singapore
| | - Shuyi Li
- Quantum Science and Engineering Centre (QSec), Nanyang Technological University, Singapore, 639798, Singapore
| | - Guanyu Chen
- Quantum Science and Engineering Centre (QSec), Nanyang Technological University, Singapore, 639798, Singapore
| | - Yuan Li
- Quantum Science and Engineering Centre (QSec), Nanyang Technological University, Singapore, 639798, Singapore
| | - Sijin Li
- Quantum Science and Engineering Centre (QSec), Nanyang Technological University, Singapore, 639798, Singapore
| | - Yunxiang Wang
- School of Optoelectronic Science and Engineering, University of Electronic Science and Technology of China, 610054, Chengdu, China
| | - Shihai Sun
- School of Electronics and Communication Engineering, Sun Yat-Sen University, 518100, Shenzhen, Guangdong, China
| | - Muhammad Faeyz Karim
- Quantum Science and Engineering Centre (QSec), Nanyang Technological University, Singapore, 639798, Singapore.
| | - Hong Cai
- Institute of Microelectronics, A*STAR (Agency for Science, Technology and Research), Singapore, 138634, Singapore.
| | - Leong Chuan Kwek
- Quantum Science and Engineering Centre (QSec), Nanyang Technological University, Singapore, 639798, Singapore.
- Centre for Quantum Technologies, National University of Singapore, 3 Science Drive 2, Singapore, 117543, Singapore.
- National Institute of Education, Nanyang Technological University, Singapore, 637616, Singapore.
| | - Ai Qun Liu
- Quantum Science and Engineering Centre (QSec), Nanyang Technological University, Singapore, 639798, Singapore.
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