Chang-Ling Zou
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The organizations/institutes from the scholar's latest article
Research Subjects
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Chang-Ling Zou has a total of 821 co-authors. Here are the top co-authors by number of shared publications:
Guang-Can Guo
University of Science and Technology of China
169 shared publications- Chun-Hua Dong
Laboratory of Quantum Information University of Science and Technology of China Hefei Anhui China
65 shared publications - Luyan Sun
Center for Quantum Information, Institute for Interdisciplinary Information Sciences, Tsinghua University, Beijing, China
60 shared publications Ming Li
Laboratory of Quantum Information, University of Science and Technology of China, Hefei 230026, China; Hefei National Laboratory, Hefei 230088, China
50 shared publicationsYan-Lei Zhang
University of Science and Technology of China
50 shared publicationsXin-Biao Xu
University of Science and Technology of China
44 shared publications
Latest Publications
- 23 October 2026
- Published by Springer Nature in Nature Physics
- p. 1-7
Beating the break-even point with autonomous quantum error correction
- 23 October 2026
- Published by Springer Nature in Nature Physics
- p. 1-7
Beating the break-even point with autonomous quantum error correction
- 24 August 2026
- Published by American Physical Society (APS) in Physical Review A
- Vol. 114 (2) , 023107
Proposal of a waveguide-integrated optical nanolens for near-field single-atom trapping
The integration of single atoms with photonic integrated circuits promises scalable quantum information platforms, yet a fundamental challenge of trapping atoms into the near-field interaction region of the waveguide mode remains. Here we propose an on-chip waveguide-based nanolens, designed to focus a free-space incident Gaussian beam, thereby creating a tight optical beam directly above the waveguide surface. In contrast to treating the diffraction effect of the on-chip nanostructure as detrimental, our approach can utilize the effect to realize precise near-field positioning and trapping of single atoms, which allows strong coupling between the trapped atom and the guided photons in the waveguide. Through numerical simulation, we demonstrate that for a free-space input of an 852-nm Gaussian beam with a waist of $1\phantom{\rule{0.28em}{0ex}}\textmu{}\mathrm{m}$, a waveguide can generate a near-field focused beam with a waist of only $0.66\phantom{\rule{0.28em}{0ex}}\textmu{}\mathrm{m}$ and a height of about $0.07\phantom{\rule{0.28em}{0ex}}\textmu{}\mathrm{m}$ above the waveguide surface, featuring a 3.0-mK dipole trap with only 3.5-mW free-space trap laser power assisted by a blue-detuned waveguide mode. The increase of atomic spontaneous emission rate induced by near-field atom-waveguide mode coupling is analyzed by the Purcell factor, which is up to $3.1\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}3}$. Furthermore, it is demonstrated that the cold atoms can be transported from the trap center of the nanolens to the optical trap arrays created by the evanescent field of the waveguide modes. Our proposal provides a scalable approach for realizing a near-field waveguide-integrated single-atom array, paving the way toward hybrid photonic-atomic circuits for quantum applications.- 24 August 2026
- Published by American Physical Society (APS) in Physical Review A
- Vol. 114 (2) , 023107
Proposal of a waveguide-integrated optical nanolens for near-field single-atom trapping
The integration of single atoms with photonic integrated circuits promises scalable quantum information platforms, yet a fundamental challenge of trapping atoms into the near-field interaction region of the waveguide mode remains. Here we propose an on-chip waveguide-based nanolens, designed to focus a free-space incident Gaussian beam, thereby creating a tight optical beam directly above the waveguide surface. In contrast to treating the diffraction effect of the on-chip nanostructure as detrimental, our approach can utilize the effect to realize precise near-field positioning and trapping of single atoms, which allows strong coupling between the trapped atom and the guided photons in the waveguide. Through numerical simulation, we demonstrate that for a free-space input of an 852-nm Gaussian beam with a waist of $1\phantom{\rule{0.28em}{0ex}}\textmu{}\mathrm{m}$, a waveguide can generate a near-field focused beam with a waist of only $0.66\phantom{\rule{0.28em}{0ex}}\textmu{}\mathrm{m}$ and a height of about $0.07\phantom{\rule{0.28em}{0ex}}\textmu{}\mathrm{m}$ above the waveguide surface, featuring a 3.0-mK dipole trap with only 3.5-mW free-space trap laser power assisted by a blue-detuned waveguide mode. The increase of atomic spontaneous emission rate induced by near-field atom-waveguide mode coupling is analyzed by the Purcell factor, which is up to $3.1\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}3}$. Furthermore, it is demonstrated that the cold atoms can be transported from the trap center of the nanolens to the optical trap arrays created by the evanescent field of the waveguide modes. Our proposal provides a scalable approach for realizing a near-field waveguide-integrated single-atom array, paving the way toward hybrid photonic-atomic circuits for quantum applications.- 20 August 2026
- Published by American Physical Society (APS) in Physical Review A
- Vol. 114 (2) , 023516
Fundamental limits of free-space microwave-to-optical frequency conversion efficiency using Rydberg atoms
Efficient microwave-to-optical frequency conversion (MOC) using Rydberg atoms is promising for radiometry, electrometry, and hybrid quantum networks. However, in free space, the total system efficiency can be much lower than the internal atomic conversion efficiency because of the large mismatch between microwave wavelength, optical wavelength, and atomic-ensemble size. Here, we develop a systematic theoretical framework in which the total conversion efficiency is factorized into microwave mode-matching efficiency, optical spin-wave extraction efficiency, and internal coherent conversion efficiency. In the regime ${\ensuremath{\lambda}}_{\mathrm{m}}\ensuremath{\gg}L\ensuremath{\gg}{\ensuremath{\lambda}}_{\mathrm{o}}$, the atomic ensemble couples to the microwave field as a collective dipole, whereas its coupling to the optical field is governed by a phase-matched spin-wave mode. We show that the total efficiency is primarily limited by microwave mode matching. For an ideal diffraction-limited Gaussian microwave mode coupled to this collective dipole, the microwave extraction factor is bounded by about $3/16$ under standard polarization and orientation averaging. This analysis provides a transparent benchmark for evaluating free-space Rydberg MOC and identifies microwave mode matching as the key target for experimental optimization.- 20 August 2026
- Published by American Physical Society (APS) in Physical Review A
- Vol. 114 (2) , 023516
Fundamental limits of free-space microwave-to-optical frequency conversion efficiency using Rydberg atoms
Efficient microwave-to-optical frequency conversion (MOC) using Rydberg atoms is promising for radiometry, electrometry, and hybrid quantum networks. However, in free space, the total system efficiency can be much lower than the internal atomic conversion efficiency because of the large mismatch between microwave wavelength, optical wavelength, and atomic-ensemble size. Here, we develop a systematic theoretical framework in which the total conversion efficiency is factorized into microwave mode-matching efficiency, optical spin-wave extraction efficiency, and internal coherent conversion efficiency. In the regime ${\ensuremath{\lambda}}_{\mathrm{m}}\ensuremath{\gg}L\ensuremath{\gg}{\ensuremath{\lambda}}_{\mathrm{o}}$, the atomic ensemble couples to the microwave field as a collective dipole, whereas its coupling to the optical field is governed by a phase-matched spin-wave mode. We show that the total efficiency is primarily limited by microwave mode matching. For an ideal diffraction-limited Gaussian microwave mode coupled to this collective dipole, the microwave extraction factor is bounded by about $3/16$ under standard polarization and orientation averaging. This analysis provides a transparent benchmark for evaluating free-space Rydberg MOC and identifies microwave mode matching as the key target for experimental optimization.- 14 August 2026
- Published by American Physical Society (APS) in Physical Review Applied
- Vol. 26 (2)
Efficient single-atom transfer from an optical conveyor belt to a tightly confined optical tweezer
- 14 August 2026
- Published by American Physical Society (APS) in Physical Review Applied
- Vol. 26 (2)
Efficient single-atom transfer from an optical conveyor belt to a tightly confined optical tweezer
- Open Access
- 3 August 2026
- Published by Springer Nature in Nature Communications
- Vol. 17 (1)
Microcomb-driven large-scale fully connected quantum network
Fully connected quantum networks enable simultaneous connection of every user to every other user and are a highly versatile and robust networking architecture. However, the scalability of such networks remains a great challenge for practical applications. Here we construct a large-scale fully connected quantum network founded on two-photon Hong-Ou-Mandel (HOM) interference, where user-to-user security is guaranteed even with an untrusted network provider. Using integrated soliton microcomb (SMC) and photonic encoding chips, we realize precise, massively parallel frequency generation and locking, high-visibility HOM interference and measurement-device-independent (MDI) quantum key distribution. The proposed architecture enables a fully connected quantum network over 200 kilometers with strict information-theoretic security via an untrusted network provider. The implemented networking architecture paves the way for large-scale fully connected MDI quantum networks across metropolitan and intercity regions.
- 3 August 2026
- Published by Springer Nature in Nature Communications
- Vol. 17 (1)
Open AccessMicrocomb-driven large-scale fully connected quantum network
Fully connected quantum networks enable simultaneous connection of every user to every other user and are a highly versatile and robust networking architecture. However, the scalability of such networks remains a great challenge for practical applications. Here we construct a large-scale fully connected quantum network founded on two-photon Hong-Ou-Mandel (HOM) interference, where user-to-user security is guaranteed even with an untrusted network provider. Using integrated soliton microcomb (SMC) and photonic encoding chips, we realize precise, massively parallel frequency generation and locking, high-visibility HOM interference and measurement-device-independent (MDI) quantum key distribution. The proposed architecture enables a fully connected quantum network over 200 kilometers with strict information-theoretic security via an untrusted network provider. The implemented networking architecture paves the way for large-scale fully connected MDI quantum networks across metropolitan and intercity regions.
- Open Access
- 1 August 2026
- Published by AIP Publishing in APL Photonics
- Vol. 11 (8)
Injection locking of photothermal oscillation in optofluidic microcavities
Optical microcavities, which exhibit ultrahigh quality factors and exceptional light-field confinement, have become an important platform for investigating nonlinear phenomena and developing highly sensitive sensors. Within these systems, photothermal oscillations induced by competing thermo-optic effects in multimaterial structures show considerable application potential. However, their practical implementation is severely limited by frequency drift and high phase noise. In this study, we demonstrate the first successful frequency stabilization of photothermal oscillation signals using electro-optic injection locking within an optofluidic microbubble resonator. Experimental results show that after locking, the linewidth of the frequency spectrum narrows markedly and the phase noise is reduced by more than 10 dB at an offset frequency of 10 Hz. Statistical analysis of 450 consecutive measurements reveals that the standard deviations of both the center frequency and peak power in the locked state are significantly lower than those in the unlocked state. This approach converts unstable photothermal oscillation signals into controlled outputs with narrow spectral bandwidth and improved phase stability. It, therefore, offers a promising strategy for overcoming signal instability, while preserving the ultrahigh sensitivity of microcavities, and provides a strong foundation for sensing applications such as biomolecule detection and environmental gas monitoring.
- 1 August 2026
- Published by AIP Publishing in APL Photonics
- Vol. 11 (8)
Open AccessInjection locking of photothermal oscillation in optofluidic microcavities
Optical microcavities, which exhibit ultrahigh quality factors and exceptional light-field confinement, have become an important platform for investigating nonlinear phenomena and developing highly sensitive sensors. Within these systems, photothermal oscillations induced by competing thermo-optic effects in multimaterial structures show considerable application potential. However, their practical implementation is severely limited by frequency drift and high phase noise. In this study, we demonstrate the first successful frequency stabilization of photothermal oscillation signals using electro-optic injection locking within an optofluidic microbubble resonator. Experimental results show that after locking, the linewidth of the frequency spectrum narrows markedly and the phase noise is reduced by more than 10 dB at an offset frequency of 10 Hz. Statistical analysis of 450 consecutive measurements reveals that the standard deviations of both the center frequency and peak power in the locked state are significantly lower than those in the unlocked state. This approach converts unstable photothermal oscillation signals into controlled outputs with narrow spectral bandwidth and improved phase stability. It, therefore, offers a promising strategy for overcoming signal instability, while preserving the ultrahigh sensitivity of microcavities, and provides a strong foundation for sensing applications such as biomolecule detection and environmental gas monitoring.
- 9 July 2026
- Published by Springer Nature in Nature Physics
- Vol. 22 (9) , 1498-1505
Principles of optics in Fock space for the scalable manipulation of large quantum states
- 9 July 2026
- Published by Springer Nature in Nature Physics
- Vol. 22 (9) , 1498-1505
Principles of optics in Fock space for the scalable manipulation of large quantum states
- 13 June 2026
- Published by Elsevier in Science Bulletin
- Vol. 71 (14) , 3544-3547
High-performance quantum interconnect between bosonic modules beyond transmission loss constraints
- 13 June 2026
- Published by Elsevier in Science Bulletin
- Vol. 71 (14) , 3544-3547
High-performance quantum interconnect between bosonic modules beyond transmission loss constraints
- 12 June 2026
- Published by IOP Publishing in Physica Scripta
- Vol. 101 (23) , 235505
A compact magnetic-free optical isolator
Current commercial optical isolators (OIs) primarily rely on the Faraday effect in magneto-optical materials, which necessitates the use of external magnetic fields. Here, we report a passive OI constructed from compact, commercially available optical components and an atomic vapor cell, which does not require a biasing magnetic field or any external drive, and only requires that the intensity of the forward beam is higher than that of the backward beam, which is very easy to satisfy in isolator applications. Operating at 795 nm, this device uses the principle of nonlinear non-reciprocity to achieve a bandwidth of 6 GHz and an isolation ratio greater than 30 dB.
- 12 June 2026
- Published by IOP Publishing in Physica Scripta
- Vol. 101 (23) , 235505
A compact magnetic-free optical isolator
Current commercial optical isolators (OIs) primarily rely on the Faraday effect in magneto-optical materials, which necessitates the use of external magnetic fields. Here, we report a passive OI constructed from compact, commercially available optical components and an atomic vapor cell, which does not require a biasing magnetic field or any external drive, and only requires that the intensity of the forward beam is higher than that of the backward beam, which is very easy to satisfy in isolator applications. Operating at 795 nm, this device uses the principle of nonlinear non-reciprocity to achieve a bandwidth of 6 GHz and an isolation ratio greater than 30 dB.
- 27 May 2026
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 136 (21) , 210602
High-Fidelity Controlled-Phase Gate for Binomial Codes via Geometric Phase Engineering
High-fidelity two-logical-qubit gates are essential for realizing fault-tolerant quantum computation with bosonic codes, yet experimentally reported fidelities have rarely exceeded 90%. Here, we propose a geometric phase engineering approach for implementing controlled-phase gates for binomially encoded logical qubits. This method leverages the structural simplicity of geometric drives to reduce the numerical optimization dimensionality while fully incorporating system nonlinearities, enabling fast and high-fidelity logical operations. As an example, we experimentally demonstrate a process fidelity of 97.4±0.8% with postselection to exclude leakage (94.9±0.7% without post selection) for a controlled-Z gate between two lowest-order binomial codes, surpassing all previously reported two-logical-qubit gates in bosonic codes. This Letter demonstrates that geometric phase engineering provides an effective and experimentally feasible route to fast, high-fidelity logical operations in bosonic quantum processors.
- 27 May 2026
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 136 (21) , 210602
High-Fidelity Controlled-Phase Gate for Binomial Codes via Geometric Phase Engineering
High-fidelity two-logical-qubit gates are essential for realizing fault-tolerant quantum computation with bosonic codes, yet experimentally reported fidelities have rarely exceeded 90%. Here, we propose a geometric phase engineering approach for implementing controlled-phase gates for binomially encoded logical qubits. This method leverages the structural simplicity of geometric drives to reduce the numerical optimization dimensionality while fully incorporating system nonlinearities, enabling fast and high-fidelity logical operations. As an example, we experimentally demonstrate a process fidelity of 97.4±0.8% with postselection to exclude leakage (94.9±0.7% without post selection) for a controlled-Z gate between two lowest-order binomial codes, surpassing all previously reported two-logical-qubit gates in bosonic codes. This Letter demonstrates that geometric phase engineering provides an effective and experimentally feasible route to fast, high-fidelity logical operations in bosonic quantum processors.