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Quantum many-body mixed phase space revealed by hybrid feedback control
Authors:
Hang Dong,
Jie Ren,
Andrew Hallam,
Han Wang,
Zhengyi Cui,
Yiren Zou,
Junlin Wang,
Hekang Li,
Qiujiang Guo,
Zhen Wang,
Lei Ying,
Zlatko Papic
Abstract:
Understanding how complex systems transition between order and chaos is a central challenge of nonequilibrium physics. While weak perturbations of classical integrable systems give rise to a mixed phase space of coexisting regular and chaotic trajectories, analogous behavior in interacting quantum many-body systems has remained elusive. Here we develop and experimentally implement a hybrid quantum…
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Understanding how complex systems transition between order and chaos is a central challenge of nonequilibrium physics. While weak perturbations of classical integrable systems give rise to a mixed phase space of coexisting regular and chaotic trajectories, analogous behavior in interacting quantum many-body systems has remained elusive. Here we develop and experimentally implement a hybrid quantum-classical feedback protocol that autonomously discovers and stabilizes long-lived regular trajectories in a superconducting quantum processor. Each iteration combines short-time quantum evolution with classical optimization that projects the dynamics back onto a low-entanglement variational manifold, effectively distilling coherence from chaotic evolution. The stabilized trajectories reveal a quantum many-body mixed phase space emerging from nonlinear variational dynamics, without a direct analogue in classical or few-body quantum systems. Our results establish a versatile framework for algorithmic discovery and control of coherent dynamics previously inaccessible to experiment.
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Submitted 15 July, 2026;
originally announced July 2026.
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A superconducting surface-code processor with lattice-surgery logical operations
Authors:
Yanzhe Wang,
Fanhao Shen,
Haipeng Xie,
Aosai Zhang,
Yu Gao,
Chuanyu Zhang,
Xuhao Zhu,
Feitong Jin,
Yiren Zou,
Ning Wang,
Zhengyi Cui,
Zehang Bao,
Zitian Zhu,
Jiarun Zhong,
Gongyu Liu,
Jia-Nan Yang,
Yihang Han,
Yiyang He,
Jiayuan Shen,
Han Wang,
Jiahua Huang,
Xinrong Zhang,
Sailang Zhou,
Hang Dong,
Jinfeng Deng
, et al. (9 additional authors not shown)
Abstract:
Fault-tolerant logical operations are fundamental for scalable quantum computation. Here, we report the experimental realization of lattice-surgery operations between a pair of distance-three surface-code logical qubits on a planar superconducting processor. During repeated syndrome extraction cycles, the logical qubits exhibit per-cycle error rates of $0.0365(2)$ and $0.0282(1)$, respectively, af…
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Fault-tolerant logical operations are fundamental for scalable quantum computation. Here, we report the experimental realization of lattice-surgery operations between a pair of distance-three surface-code logical qubits on a planar superconducting processor. During repeated syndrome extraction cycles, the logical qubits exhibit per-cycle error rates of $0.0365(2)$ and $0.0282(1)$, respectively, after leakage events are rejected. By leveraging joint initialization and lattice splitting, we deterministically prepare a logical Bell state, confirming genuine bipartite entanglement via the error-corrected logical state fidelity. We further execute a two-qubit Deutsch-Jozsa algorithm at the logical level to demonstrate algorithmic utility in a fault-tolerant framework. Finally, to achieve universal control, we implement magic-state injection and gate teleportation to realize continuous non-Clifford rotations about the logical $X$ axis. For the logical $R_{X}(π/4)$ gate, we achieve a logical gate fidelity of $0.943_{-9}^{+10}$ conditioned on the absence of detected errors. These results establish lattice surgery as a practical and versatile paradigm for logical computation in near-term surface-code architectures, representing a critical milestone toward scalable fault-tolerant quantum advantage in superconducting circuits.
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Submitted 4 June, 2026;
originally announced June 2026.
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Phase diagram of a dual-species Rydberg atom ladder
Authors:
Lei-Yi-Nan Liu,
Shi-Rong Peng,
Ze-Yuan Huang,
Xing-Man Wei,
Yun-Han Zou,
Su Yi,
Jian Cui
Abstract:
Dual-species Rydberg atom arrays extend single-species platforms by introducing competing interaction scales and enhanced quantum fluctuations, enabling phenomena beyond homogeneous settings. In this work, we study the ground-state phase diagram of a one-dimensional dual-species Rydberg atom ladder using large-scale density-matrix renormalization group calculations. We identify disordered phases,…
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Dual-species Rydberg atom arrays extend single-species platforms by introducing competing interaction scales and enhanced quantum fluctuations, enabling phenomena beyond homogeneous settings. In this work, we study the ground-state phase diagram of a one-dimensional dual-species Rydberg atom ladder using large-scale density-matrix renormalization group calculations. We identify disordered phases, multiple ordered phases with $\mathbb{Z}_2$, $\mathbb{Z}_3$, and $\mathbb{Z}_4$ symmetry, as well as floating phases characterized by incommensurate wave vectors and algebraically decaying correlations. Importantly, we observe a smooth crossover between distinct $\mathbb{Z}_2$-ordered regimes, reflecting a reorganization of low-energy degrees of freedom rather than a true phase transition, which is absent in single-species Rydberg arrays. We further uncover a multi-critical point at the boundary between the $\mathbb{Z}_2 \otimes \mathbb{Z}_2$ and $\mathbb{Z}_3 \otimes \mathbb{Z}_3$ ordered phases, where Ising, chiral, and first-order transition lines intersect. Our results demonstrate that dual-species Rydberg atom arrays provide a unique platform for realizing crossover physics and multi-critical behavior inaccessible in single-species architectures.
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Submitted 27 April, 2026;
originally announced April 2026.
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Teleportation transition of surface codes on a superconducting quantum processor
Authors:
Yiren Zou,
Hong-Kuan Xia,
Aosai Zhang,
Xuhao Zhu,
Feitong Jin,
Qingyuan Wang,
Yu Gao,
Chuanyu Zhang,
Ning Wang,
Zhengyi Cui,
Fanhao Shen,
Zehang Bao,
Zitian Zhu,
Jiarun Zhong,
Gongyu Liu,
Jia-Nan Yang,
Yihang Han,
Yiyang He,
Jiayuan Shen,
Han Wang,
Yanzhe Wang,
Jiahua Huang,
Xinrong Zhang,
Sailang Zhou,
Hang Dong
, et al. (10 additional authors not shown)
Abstract:
The topological surface code is a leading candidate for harnessing long-range entanglement to protect logical quantum information against errors, and teleportation of logical states is desirable for robust quantum information processing. Nevertheless, scaling up the surface code in quantum teleportation poses a formidable challenge to experiment. Here on a superconducting quantum processor with 12…
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The topological surface code is a leading candidate for harnessing long-range entanglement to protect logical quantum information against errors, and teleportation of logical states is desirable for robust quantum information processing. Nevertheless, scaling up the surface code in quantum teleportation poses a formidable challenge to experiment. Here on a superconducting quantum processor with 125 qubits, we demonstrate the robust teleportation of topological rotated surface code prepared by a linear-depth unitary circuit, with code distances up to 7. We obtain the teleportation phase diagram by tuning the local entangling gates uniformly across a finite threshold. Furthermore, we show that the entangling threshold can be boosted by coherent qubit rotations that inject magic resources beyond the Clifford regime, restoring the duality symmetry of the topological phase, which serves as a guiding principle to minimize the entanglement resource. Our results shed light on simulating and leveraging topological quantum matter on quantum devices, and pave the way to the ultimate goal of distributed fault tolerant quantum computation.
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Submitted 24 February, 2026;
originally announced February 2026.
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Unlearnable phases of matter
Authors:
Tarun Advaith Kumar,
Yijian Zou,
Amir-Reza Negari,
Roger G. Melko,
Timothy H. Hsieh
Abstract:
We identify fundamental limitations in machine learning by demonstrating that non-trivial mixed-state phases of matter are computationally hard to learn. Focusing on unsupervised learning of distributions, we show that autoregressive neural networks fail to learn global properties of distributions characterized by locally indistinguishable (LI) states. We demonstrate that conditional mutual inform…
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We identify fundamental limitations in machine learning by demonstrating that non-trivial mixed-state phases of matter are computationally hard to learn. Focusing on unsupervised learning of distributions, we show that autoregressive neural networks fail to learn global properties of distributions characterized by locally indistinguishable (LI) states. We demonstrate that conditional mutual information (CMI) is a useful diagnostic for LI: we show that for classical distributions, long-range CMI of a state implies a spatially LI partner. By introducing a restricted statistical query model, we prove that nontrivial phases with long-range CMI, such as strong-to-weak spontaneous symmetry breaking phases, are hard to learn. We validate our claims by using recurrent, convolutional, and Transformer neural networks to learn the syndrome and physical distributions of toric/surface code under bit flip noise. Our findings suggest hardness of learning as a diagnostic tool for detecting mixed-state phases and transitions and error-correction thresholds, and they suggest CMI and more generally ``non-local Gibbsness'' as metrics for how hard a distribution is to learn.
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Submitted 18 March, 2026; v1 submitted 11 February, 2026;
originally announced February 2026.
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Polynomial-time certification of fidelity for many-body mixed states and mixed-state universality classes
Authors:
Yuhan Liu,
Yijian Zou
Abstract:
Computation of Uhlmann fidelity between many-body mixed states generally involves full diagonalization of exponentially large matrices. In this work, we introduce a polynomial-time algorithm to compute certified lower and upper bounds for the fidelity between matrix product density operators (MPDOs). Our method maps the fidelity estimation problem to a variational optimization of sequential quantu…
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Computation of Uhlmann fidelity between many-body mixed states generally involves full diagonalization of exponentially large matrices. In this work, we introduce a polynomial-time algorithm to compute certified lower and upper bounds for the fidelity between matrix product density operators (MPDOs). Our method maps the fidelity estimation problem to a variational optimization of sequential quantum circuits, allowing for systematic improvement of the lower bounds by increasing the circuit depth. Complementarily, we obtain certified upper bounds on fidelity by variational lower bounds on the trace distance through the same framework. We demonstrate the power of this approach with two examples: fidelity correlators in critical mixed states, and codeword distinguishability in an approximate quantum error-correcting code. Remarkably, the variational lower bound accurately track the universal scaling behavior of the fidelity with a size-consistent relative error, allowing for the extraction of previously unknown critical exponents. Our results offer an exponential improvement in precision over known moment-based bounds and establish a scalable framework for the verification of many-body quantum systems.
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Submitted 19 January, 2026;
originally announced January 2026.
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El Agente Cuantico: Automating quantum simulations
Authors:
Ignacio Gustin,
Luis Mantilla Calderón,
Juan B. Pérez-Sánchez,
Jérôme F. Gonthier,
Yuma Nakamura,
Karthik Panicker,
Manav Ramprasad,
Zijian Zhang,
Yunheng Zou,
Varinia Bernales,
Alán Aspuru-Guzik
Abstract:
Quantum simulation is central to understanding and designing quantum systems across physics and chemistry. Yet it has barriers to access from both computational complexity and computational perspectives, due to the exponential growth of Hilbert space and the complexity of modern software tools. Here we introduce{\cinzel El Agente Cuántico}, a multi-agent AI system that automates quantum-simulation…
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Quantum simulation is central to understanding and designing quantum systems across physics and chemistry. Yet it has barriers to access from both computational complexity and computational perspectives, due to the exponential growth of Hilbert space and the complexity of modern software tools. Here we introduce{\cinzel El Agente Cuántico}, a multi-agent AI system that automates quantum-simulation workflows by translating natural-language scientific intent into executed and validated computations across heterogeneous quantum-software frameworks. By reasoning directly over library documentation and APIs, our agentic system dynamically assembles end-to-end simulations spanning state preparation, closed- and open-system dynamics, tensor-network methods, quantum control, quantum error correction, and quantum resource estimation. The developed system unifies traditionally distinct simulation paradigms behind a single natural-language interface. Beyond reducing technical barriers, this approach opens a path toward scalable, adaptive, and increasingly autonomous quantum simulation, enabling faster exploration of physical models, rapid hypothesis testing, and closer integration between theory, simulation, and emerging quantum hardware.
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Submitted 5 March, 2026; v1 submitted 21 December, 2025;
originally announced December 2025.
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Fock space prethermalization and time-crystalline order on a quantum processor
Authors:
Zehang Bao,
Zitian Zhu,
Yang-Ren Liu,
Zixuan Song,
Feitong Jin,
Xuhao Zhu,
Yu Gao,
Chuanyu Zhang,
Ning Wang,
Yiren Zou,
Ziqi Tan,
Aosai Zhang,
Zhengyi Cui,
Fanhao Shen,
Jiarun Zhong,
Yiyang He,
Han Wang,
Jia-Nan Yang,
Yanzhe Wang,
Jiayuan Shen,
Gongyu Liu,
Yihang Han,
Yaozu Wu,
Jinfeng Deng,
Hang Dong
, et al. (9 additional authors not shown)
Abstract:
Periodically driven quantum many-body systems exhibit a wide variety of exotic nonequilibrium phenomena and provide a promising pathway for quantum applications. A fundamental challenge for stabilizing and harnessing these highly entangled states of matter is system heating by energy absorption from the drive. Here, we propose and demonstrate a disorder-free mechanism, dubbed Fock space prethermal…
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Periodically driven quantum many-body systems exhibit a wide variety of exotic nonequilibrium phenomena and provide a promising pathway for quantum applications. A fundamental challenge for stabilizing and harnessing these highly entangled states of matter is system heating by energy absorption from the drive. Here, we propose and demonstrate a disorder-free mechanism, dubbed Fock space prethermalization (FSP), to suppress heating. This mechanism divides the Fock-space network into linearly many sparse sub-networks, thereby prolonging the thermalization timescale even for initial states at high energy densities. Using 72 superconducting qubits, we observe an FSP-based time-crystalline order that persists over 120 cycles for generic initial Fock states. The underlying kinetic constraint of approximately conserved domain wall (DW) numbers is identified by measuring site-resolved correlators. Further, we perform finite-size scaling analysis for DW and Fock-space dynamics by varying system sizes, which reveals size-independent regimes for FSP-thermalization crossover and links the dynamical behaviors to the eigenstructure of the Floquet unitary. Our work establishes FSP as a robust mechanism for breaking ergodicity, and paves the way for exploring novel nonequilibrium quantum matter and its applications.
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Submitted 18 March, 2026; v1 submitted 28 October, 2025;
originally announced October 2025.
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Combinatorial optimization enhanced by shallow quantum circuits with 104 superconducting qubits
Authors:
Xuhao Zhu,
Zuoheng Zou,
Feitong Jin,
Pavel Mosharev,
Maolin Luo,
Yaozu Wu,
Jiachen Chen,
Chuanyu Zhang,
Yu Gao,
Ning Wang,
Yiren Zou,
Aosai Zhang,
Fanhao Shen,
Zehang Bao,
Zitian Zhu,
Jiarun Zhong,
Zhengyi Cui,
Yihang Han,
Yiyang He,
Han Wang,
Jia-Nan Yang,
Yanzhe Wang,
Jiayuan Shen,
Gongyu Liu,
Zixuan Song
, et al. (9 additional authors not shown)
Abstract:
A pivotal task for quantum computing is to speed up solving problems that are both classically intractable and practically valuable. Among these, combinatorial optimization problems have attracted tremendous attention due to their broad applicability and natural fitness to Ising Hamiltonians. Here we propose a quantum sampling strategy, based on which we design an algorithm for accelerating solvin…
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A pivotal task for quantum computing is to speed up solving problems that are both classically intractable and practically valuable. Among these, combinatorial optimization problems have attracted tremendous attention due to their broad applicability and natural fitness to Ising Hamiltonians. Here we propose a quantum sampling strategy, based on which we design an algorithm for accelerating solving the ground states of Ising model, a class of NP-hard problems in combinatorial optimization. The algorithm employs a hybrid quantum-classical workflow, with a shallow-circuit quantum sampling subroutine dedicated to navigating the energy landscape. Using up to 104 superconducting qubits, we demonstrate that this algorithm outputs favorable solutions against even a highly-optimized classical simulated annealing (SA) algorithm. Furthermore, we illustrate the path toward quantum speedup based on the time-to-solution metric against SA running on a single-core CPU with just 100 qubits. Our results indicate a promising alternative to classical heuristics for combinatorial optimization, a paradigm where quantum advantage might become possible on near-term superconducting quantum processors with thousands of qubits and without the assistance of error correction.
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Submitted 14 September, 2025;
originally announced September 2025.
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Universal quantum phase classification on quantum computers from machine learning
Authors:
Weicheng Ye,
Shuwei Liu,
Shiyu Zhou,
Yijian Zou
Abstract:
The classification of quantum phases of matter remains a fundamental challenge in condensed matter physics. We present a novel framework that combines shadow tomography with modern time-series machine learning models to enable efficient and practical quantum phase classification. Our approach leverages the definition of quantum phases based on connectivity through finite-depth local unitary circui…
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The classification of quantum phases of matter remains a fundamental challenge in condensed matter physics. We present a novel framework that combines shadow tomography with modern time-series machine learning models to enable efficient and practical quantum phase classification. Our approach leverages the definition of quantum phases based on connectivity through finite-depth local unitary circuits, generating abundant training data by applying Haar random evolution to representative quantum states for a given phase. In this way, the training data can be efficiently obtained from a quantum simulator. Additionally, we demonstrate that advanced time-series models can be used to process the training data and achieve universal quantum phase classification that does not rely on local order parameters. To validate the universality and versatility of our method, we test the model against one-dimensional quantum spin chains such as the Ising model and the axial next-nearest-neighbor Ising (ANNNI) model, showing excellent agreement with known phase boundaries.
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Submitted 6 August, 2025;
originally announced August 2025.
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Experimental realization of the bucket-brigade quantum random access memory
Authors:
Fanhao Shen,
Yujie Ji,
Debin Xiang,
Yanzhe Wang,
Ke Wang,
Chuanyu Zhang,
Aosai Zhang,
Yiren Zou,
Yu Gao,
Zhengyi Cui,
Gongyu Liu,
Jianan Yang,
Yihang Han,
Jinfeng Deng,
Anbang Wang,
Zhihong Zhang,
Hekang Li,
Qiujiang Guo,
Pengfei Zhang,
Chao Song,
Liqiang Lu,
Zhen Wang,
Jianwei Yin
Abstract:
Quantum random access memory (QRAM) enables efficient classical data access for quantum computers -- a prerequisite for many quantum algorithms to achieve quantum speedup. Despite various proposals, the experimental realization of QRAM remains largely unexplored. Here, we experimentally investigate the circuit-based bucket-brigade QRAM with a superconducting quantum processor. To facilitate the ex…
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Quantum random access memory (QRAM) enables efficient classical data access for quantum computers -- a prerequisite for many quantum algorithms to achieve quantum speedup. Despite various proposals, the experimental realization of QRAM remains largely unexplored. Here, we experimentally investigate the circuit-based bucket-brigade QRAM with a superconducting quantum processor. To facilitate the experimental implementation, we introduce a hardware-efficient gate decomposition scheme for quantum routers, which effectively reduces the depth of the QRAM circuit by more than 30% compared to the conventional controlled-SWAP-based implementation. We further propose an error mitigation method to boost the QRAM query fidelity. With these techniques, we are able to experimentally implement the QRAM architectures with two and three layers, achieving query fidelities up to 0.800 $\pm$ 0.026 and 0.604$\pm$0.005, respectively. Additionally, we study the error propagation mechanism and the scalability of our QRAM implementation, providing experimental evidence for the noise resilience nature of the bucket-brigade QRAM architecture. Our results highlight the potential of superconducting quantum processors for realizing a scalable QRAM architecture.
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Submitted 19 June, 2025;
originally announced June 2025.
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Demonstration of low-overhead quantum error correction codes
Authors:
Ke Wang,
Zhide Lu,
Chuanyu Zhang,
Gongyu Liu,
Jiachen Chen,
Yanzhe Wang,
Yaozu Wu,
Shibo Xu,
Xuhao Zhu,
Feitong Jin,
Yu Gao,
Ziqi Tan,
Zhengyi Cui,
Ning Wang,
Yiren Zou,
Aosai Zhang,
Tingting Li,
Fanhao Shen,
Jiarun Zhong,
Zehang Bao,
Zitian Zhu,
Yihang Han,
Yiyang He,
Jiayuan Shen,
Han Wang
, et al. (17 additional authors not shown)
Abstract:
Quantum computers hold the potential to surpass classical computers in solving complex computational problems. However, the fragility of quantum information and the error-prone nature of quantum operations make building large-scale, fault-tolerant quantum computers a prominent challenge. To combat errors, pioneering experiments have demonstrated a variety of quantum error correction codes. Yet, mo…
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Quantum computers hold the potential to surpass classical computers in solving complex computational problems. However, the fragility of quantum information and the error-prone nature of quantum operations make building large-scale, fault-tolerant quantum computers a prominent challenge. To combat errors, pioneering experiments have demonstrated a variety of quantum error correction codes. Yet, most of these codes suffer from low encoding efficiency, and their scalability is hindered by prohibitively high resource overheads. Here, we report the demonstration of two low-overhead quantum low-density parity-check (qLDPC) codes, a distance-4 bivariate bicycle code and a distance-3 qLDPC code, on our latest superconducting processor, Kunlun, featuring 32 long-range-coupled transmon qubits. Utilizing a two-dimensional architecture with overlapping long-range couplers, we demonstrate simultaneous measurements of all nonlocal weight-6 stabilizers via the periodic execution of an efficient syndrome extraction circuit. We achieve a logical error rate per logical qubit per cycle of $(8.91 \pm 0.17)\%$ for the distance-4 bivariate bicycle code with four logical qubits and $(7.77 \pm 0.12)\%$ for the distance-3 qLDPC code with six logical qubits. Our results establish the feasibility of implementing various qLDPC codes with long-range coupled superconducting processors, marking a crucial step towards large-scale low-overhead quantum error correction.
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Submitted 14 May, 2025;
originally announced May 2025.
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Probing mixed-state phases on a quantum computer via Renyi correlators and variational decoding
Authors:
Yuxuan Zhang,
Timothy H. Hsieh,
Yong Baek Kim,
Yijian Zou
Abstract:
Recent advances have defined nontrivial phases of matter in open quantum systems, such as many-body quantum states subject to environmental noise. In this work, we experimentally probe and characterize mixed-state phases on Quantinuum's H1 quantum computer using two measures: Renyi correlators and the coding performance of a quantum error-correcting code associated with the phase. As a concrete ex…
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Recent advances have defined nontrivial phases of matter in open quantum systems, such as many-body quantum states subject to environmental noise. In this work, we experimentally probe and characterize mixed-state phases on Quantinuum's H1 quantum computer using two measures: Renyi correlators and the coding performance of a quantum error-correcting code associated with the phase. As a concrete example, we probe the low-energy states of the critical transverse field Ising model under different dephasing noise channels. First, we employ shadow tomography to observe a newly proposed Renyi correlator in two distinct phases: one exhibiting power-law decay and the other long-ranged. Second, we investigate the decoding fidelity of the associated quantum error-correcting code using a variational quantum circuit, and we find that a shallow circuit is sufficient to distinguish the above-mentioned two mixed-state phases through the decoding performance quantified by entanglement fidelity. Our work is a proof of concept for the quantum simulation and characterization of mixed-state phases.
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Submitted 5 May, 2025;
originally announced May 2025.
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Quantum ensemble learning with a programmable superconducting processor
Authors:
Jiachen Chen,
Yaozu Wu,
Zhen Yang,
Shibo Xu,
Xuan Ye,
Daili Li,
Ke Wang,
Chuanyu Zhang,
Feitong Jin,
Xuhao Zhu,
Yu Gao,
Ziqi Tan,
Zhengyi Cui,
Aosai Zhang,
Ning Wang,
Yiren Zou,
Tingting Li,
Fanhao Shen,
Jiarun Zhong,
Zehang Bao,
Zitian Zhu,
Zixuan Song,
Jinfeng Deng,
Hang Dong,
Pengfei Zhang
, et al. (8 additional authors not shown)
Abstract:
Quantum machine learning is among the most exciting potential applications of quantum computing. However, the vulnerability of quantum information to environmental noises and the consequent high cost for realizing fault tolerance has impeded the quantum models from learning complex datasets. Here, we introduce AdaBoost.Q, a quantum adaptation of the classical adaptive boosting (AdaBoost) algorithm…
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Quantum machine learning is among the most exciting potential applications of quantum computing. However, the vulnerability of quantum information to environmental noises and the consequent high cost for realizing fault tolerance has impeded the quantum models from learning complex datasets. Here, we introduce AdaBoost.Q, a quantum adaptation of the classical adaptive boosting (AdaBoost) algorithm designed to enhance learning capabilities of quantum classifiers. Based on the probabilistic nature of quantum measurement, the algorithm improves the prediction accuracy by refining the attention mechanism during the adaptive training and combination of quantum classifiers. We experimentally demonstrate the versatility of our approach on a programmable superconducting processor, where we observe notable performance enhancements across various quantum machine learning models, including quantum neural networks and quantum convolutional neural networks. With AdaBoost.Q, we achieve an accuracy above 86% for a ten-class classification task over 10,000 test samples, and an accuracy of 100% for a quantum feature recognition task over 1,564 test samples. Our results demonstrate a foundational tool for advancing quantum machine learning towards practical applications, which has broad applicability to both the current noisy and the future fault-tolerant quantum devices.
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Submitted 13 March, 2025;
originally announced March 2025.
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Chirality, magic, and quantum correlations in multipartite quantum states
Authors:
Shreya Vardhan,
Bowen Shi,
Isaac H. Kim,
Yijian Zou
Abstract:
We introduce a notion of chirality for generic quantum states. A chiral state is defined as a state which cannot be transformed into its complex conjugate in a local product basis using local unitary operations. We introduce a number of quantitative measures of chirality which vanish for non-chiral states. A faithful measure called the "chiral log-distance" is defined in terms of the maximum fidel…
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We introduce a notion of chirality for generic quantum states. A chiral state is defined as a state which cannot be transformed into its complex conjugate in a local product basis using local unitary operations. We introduce a number of quantitative measures of chirality which vanish for non-chiral states. A faithful measure called the "chiral log-distance" is defined in terms of the maximum fidelity between the state and its complex conjugate under local unitary transformations. We further introduce a set of computable measures that involve nested commutators of modular Hamiltonians. We show general relations between chirality and the amount of "magic" or non-stabilizer resource in a state. We first show that stabilizer states of qubits are non-chiral. Furthermore, magic monotones such as the stabilizer nullity and the stabilizer fidelity are lower-bounded by the chiral log-distance. We further relate chirality to discord-like quantum correlations. We define a measure of discord-like correlations called the intrinsic interferometric power, and show that it is lower-bounded by a nested commutator chirality measure. One interesting aspect of chirality is that it is not monotonic under local partial traces, indicating that it is a unique kind of resource that is not captured by traditional quantum resource theories.
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Submitted 13 March, 2025;
originally announced March 2025.
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Universal Properties of Critical Mixed States from Measurement and Feedback
Authors:
Zhehao Zhang,
Yijian Zou,
Timothy H. Hsieh,
Sagar Vijay
Abstract:
We explore the universal properties of mixed quantum matter obtained from "single-shot" adaptive evolution, in which a quantum-critical ground-state is manipulated through a single round of local measurements and local unitary operations conditioned on spatially-distant measurement outcomes. The resulting mixed quantum states are characterized by altered long-distance correlations between local ob…
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We explore the universal properties of mixed quantum matter obtained from "single-shot" adaptive evolution, in which a quantum-critical ground-state is manipulated through a single round of local measurements and local unitary operations conditioned on spatially-distant measurement outcomes. The resulting mixed quantum states are characterized by altered long-distance correlations between local observables, mixed-state entropy, and entanglement negativity. By invoking a coarse-grained, continuum description of single-shot adaptation in (1+1) dimensions, we find that the extensive mixed-state entropy exhibits a sub-leading, constant correction ($γ$), while the entanglement negativity can grow logarithmically with sub-region size, with a coefficient ($α$); both constants can attain universal values which are distinct from the expected behavior in any quantum-critical ground-state. We investigate these properties in single-shot adaptation on ($i$) the critical point between a one-dimensional $Z_{2}\times Z_{2}$ symmetry-protected topological (SPT) order and a symmetry-broken state, and ($ii$) a spinful Tomonaga-Luttinger liquid. In the former case, adaptive evolution that decoheres one sublattice of the SPT can yield a critical mixed-state in which $α$ attains a universal value, which is half of that in the original state. In the latter case, we show how adaptation -- involving feedback on the spin degrees of freedom, after measuring the local charge -- modifies long-distance correlations, and determine via an exact replica field-theoretic calculation that $α$ and $γ$ vary continuously with the strength of feedback. Numerical studies confirm these results.
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Submitted 12 March, 2025;
originally announced March 2025.
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Demonstrating quantum error mitigation on logical qubits
Authors:
Aosai Zhang,
Haipeng Xie,
Yu Gao,
Jia-Nan Yang,
Zehang Bao,
Zitian Zhu,
Jiachen Chen,
Ning Wang,
Chuanyu Zhang,
Jiarun Zhong,
Shibo Xu,
Ke Wang,
Yaozu Wu,
Feitong Jin,
Xuhao Zhu,
Yiren Zou,
Ziqi Tan,
Zhengyi Cui,
Fanhao Shen,
Tingting Li,
Yihang Han,
Yiyang He,
Gongyu Liu,
Jiayuan Shen,
Han Wang
, et al. (10 additional authors not shown)
Abstract:
A long-standing challenge in quantum computing is developing technologies to overcome the inevitable noise in qubits. To enable meaningful applications in the early stages of fault-tolerant quantum computing, devising methods to suppress post-correction logical failures is becoming increasingly crucial. In this work, we propose and experimentally demonstrate the application of zero-noise extrapola…
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A long-standing challenge in quantum computing is developing technologies to overcome the inevitable noise in qubits. To enable meaningful applications in the early stages of fault-tolerant quantum computing, devising methods to suppress post-correction logical failures is becoming increasingly crucial. In this work, we propose and experimentally demonstrate the application of zero-noise extrapolation, a practical quantum error mitigation technique, to error correction circuits on state-of-the-art superconducting processors. By amplifying the noise on physical qubits, the circuits yield outcomes that exhibit a predictable dependence on noise strength, following a polynomial function determined by the code distance. This property enables the effective application of polynomial extrapolation to mitigate logical errors. Our experiments demonstrate a universal reduction in logical errors across various quantum circuits, including fault-tolerant circuits of repetition and surface codes. We observe a favorable performance in multi-round error correction circuits, indicating that this method remains effective when the circuit depth increases. These results advance the frontier of quantum error suppression technologies, opening a practical way to achieve reliable quantum computing in the early fault-tolerant era.
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Submitted 15 January, 2025;
originally announced January 2025.
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Observation of topological prethermal strong zero modes
Authors:
Feitong Jin,
Si Jiang,
Xuhao Zhu,
Zehang Bao,
Fanhao Shen,
Ke Wang,
Zitian Zhu,
Shibo Xu,
Zixuan Song,
Jiachen Chen,
Ziqi Tan,
Yaozu Wu,
Chuanyu Zhang,
Yu Gao,
Ning Wang,
Yiren Zou,
Aosai Zhang,
Tingting Li,
Jiarun Zhong,
Zhengyi Cui,
Yihang Han,
Yiyang He,
Han Wang,
Jianan Yang,
Yanzhe Wang
, et al. (20 additional authors not shown)
Abstract:
Symmetry-protected topological phases cannot be described by any local order parameter and are beyond the conventional symmetry-breaking paradigm for understanding quantum matter. They are characterized by topological boundary states robust against perturbations that respect the protecting symmetry. In a clean system without disorder, these edge modes typically only occur for the ground states of…
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Symmetry-protected topological phases cannot be described by any local order parameter and are beyond the conventional symmetry-breaking paradigm for understanding quantum matter. They are characterized by topological boundary states robust against perturbations that respect the protecting symmetry. In a clean system without disorder, these edge modes typically only occur for the ground states of systems with a bulk energy gap and would not survive at finite temperatures due to mobile thermal excitations. Here, we report the observation of a distinct type of topological edge modes, which are protected by emergent symmetries and persist even up to infinite temperature, with an array of 100 programmable superconducting qubits. In particular, through digital quantum simulation of the dynamics of a one-dimensional disorder-free "cluster" Hamiltonian, we observe robust long-lived topological edge modes over up to 30 cycles at a wide range of temperatures. By monitoring the propagation of thermal excitations, we show that despite the free mobility of these excitations, their interactions with the edge modes are substantially suppressed in the dimerized regime due to an emergent U(1)$\times$U(1) symmetry, resulting in an unusually prolonged lifetime of the topological edge modes even at infinite temperature. In addition, we exploit these topological edge modes as logical qubits and prepare a logical Bell state, which exhibits persistent coherence in the dimerized and off-resonant regime, despite the system being disorder-free and far from its ground state. Our results establish a viable digital simulation approach to experimentally exploring a variety of finite-temperature topological phases and demonstrate a potential route to construct long-lived robust boundary qubits that survive to infinite temperature in disorder-free systems.
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Submitted 8 January, 2025;
originally announced January 2025.
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Exploring nontrivial topology at quantum criticality in a superconducting processor
Authors:
Ziqi Tan,
Ke Wang,
Sheng Yang,
Fanhao Shen,
Feitong Jin,
Xuhao Zhu,
Yujie Ji,
Shibo Xu,
Jiachen Chen,
Yaozu Wu,
Chuanyu Zhang,
Yu Gao,
Ning Wang,
Yiren Zou,
Aosai Zhang,
Tingting Li,
Zehang Bao,
Zitian Zhu,
Jiarun Zhong,
Zhengyi Cui,
Yihang Han,
Yiyang He,
Han Wang,
Jianan Yang,
Yanzhe Wang
, et al. (15 additional authors not shown)
Abstract:
The discovery of nontrivial topology in quantum critical states has introduced a new paradigm for classifying quantum phase transitions and challenges the conventional belief that topological phases are typically associated with a bulk energy gap. However, realizing and characterizing such topologically nontrivial quantum critical states with large particle numbers remains an outstanding experimen…
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The discovery of nontrivial topology in quantum critical states has introduced a new paradigm for classifying quantum phase transitions and challenges the conventional belief that topological phases are typically associated with a bulk energy gap. However, realizing and characterizing such topologically nontrivial quantum critical states with large particle numbers remains an outstanding experimental challenge in statistical and condensed matter physics. Programmable quantum processors can directly prepare and manipulate exotic quantum many-body states, offering a powerful path for exploring the physics behind these states. Here, we present an experimental exploration of the critical cluster Ising model by preparing its low-lying critical states on a superconducting processor with up to $100$ qubits. We develop an efficient method to probe the boundary $g$-function based on prepared low-energy states, which allows us to uniquely identify the nontrivial topology of the critical systems under study. Furthermore, by adapting the entanglement Hamiltonian tomography technique, we recognize two-fold topological degeneracy in the entanglement spectrum under periodic boundary condition, experimentally verifying the universal bulk-boundary correspondence in topological critical systems. Our results demonstrate the low-lying critical states as useful quantum resources for investigating the interplay between topology and quantum criticality.
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Submitted 8 January, 2025;
originally announced January 2025.
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Emergence of steady quantum transport in a superconducting processor
Authors:
Pengfei Zhang,
Yu Gao,
Xiansong Xu,
Ning Wang,
Hang Dong,
Chu Guo,
Jinfeng Deng,
Xu Zhang,
Jiachen Chen,
Shibo Xu,
Ke Wang,
Yaozu Wu,
Chuanyu Zhang,
Feitong Jin,
Xuhao Zhu,
Aosai Zhang,
Yiren Zou,
Ziqi Tan,
Zhengyi Cui,
Zitian Zhu,
Fanhao Shen,
Tingting Li,
Jiarun Zhong,
Zehang Bao,
Liangtian Zhao
, et al. (7 additional authors not shown)
Abstract:
Non-equilibrium quantum transport is crucial to technological advances ranging from nanoelectronics to thermal management. In essence, it deals with the coherent transfer of energy and (quasi-)particles through quantum channels between thermodynamic baths. A complete understanding of quantum transport thus requires the ability to simulate and probe macroscopic and microscopic physics on equal foot…
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Non-equilibrium quantum transport is crucial to technological advances ranging from nanoelectronics to thermal management. In essence, it deals with the coherent transfer of energy and (quasi-)particles through quantum channels between thermodynamic baths. A complete understanding of quantum transport thus requires the ability to simulate and probe macroscopic and microscopic physics on equal footing. Using a superconducting quantum processor, we demonstrate the emergence of non-equilibrium steady quantum transport by emulating the baths with qubit ladders and realising steady particle currents between the baths. We experimentally show that the currents are independent of the microscopic details of bath initialisation, and their temporal fluctuations decrease rapidly with the size of the baths, emulating those predicted by thermodynamic baths. The above characteristics are experimental evidence of pure-state statistical mechanics and prethermalisation in non-equilibrium many-body quantum systems. Furthermore, by utilising precise controls and measurements with single-site resolution, we demonstrate the capability to tune steady currents by manipulating the macroscopic properties of the baths, including filling and spectral properties. Our investigation paves the way for a new generation of experimental exploration of non-equilibrium quantum transport in strongly correlated quantum matter.
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Submitted 11 November, 2024;
originally announced November 2024.
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Quantum continual learning on a programmable superconducting processor
Authors:
Chuanyu Zhang,
Zhide Lu,
Liangtian Zhao,
Shibo Xu,
Weikang Li,
Ke Wang,
Jiachen Chen,
Yaozu Wu,
Feitong Jin,
Xuhao Zhu,
Yu Gao,
Ziqi Tan,
Zhengyi Cui,
Aosai Zhang,
Ning Wang,
Yiren Zou,
Tingting Li,
Fanhao Shen,
Jiarun Zhong,
Zehang Bao,
Zitian Zhu,
Zixuan Song,
Jinfeng Deng,
Hang Dong,
Pengfei Zhang
, et al. (10 additional authors not shown)
Abstract:
Quantum computers may outperform classical computers on machine learning tasks. In recent years, a variety of quantum algorithms promising unparalleled potential to enhance, speed up, or innovate machine learning have been proposed. Yet, quantum learning systems, similar to their classical counterparts, may likewise suffer from the catastrophic forgetting problem, where training a model with new t…
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Quantum computers may outperform classical computers on machine learning tasks. In recent years, a variety of quantum algorithms promising unparalleled potential to enhance, speed up, or innovate machine learning have been proposed. Yet, quantum learning systems, similar to their classical counterparts, may likewise suffer from the catastrophic forgetting problem, where training a model with new tasks would result in a dramatic performance drop for the previously learned ones. This problem is widely believed to be a crucial obstacle to achieving continual learning of multiple sequential tasks. Here, we report an experimental demonstration of quantum continual learning on a fully programmable superconducting processor. In particular, we sequentially train a quantum classifier with three tasks, two about identifying real-life images and the other on classifying quantum states, and demonstrate its catastrophic forgetting through experimentally observed rapid performance drops for prior tasks. To overcome this dilemma, we exploit the elastic weight consolidation strategy and show that the quantum classifier can incrementally learn and retain knowledge across the three distinct tasks, with an average prediction accuracy exceeding 92.3%. In addition, for sequential tasks involving quantum-engineered data, we demonstrate that the quantum classifier can achieve a better continual learning performance than a commonly used classical feedforward network with a comparable number of variational parameters. Our results establish a viable strategy for empowering quantum learning systems with desirable adaptability to multiple sequential tasks, marking an important primary experimental step towards the long-term goal of achieving quantum artificial general intelligence.
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Submitted 15 September, 2024;
originally announced September 2024.
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Quantum highway: Observation of minimal and maximal speed limits for few and many-body states
Authors:
Zitian Zhu,
Lei Gao,
Zehang Bao,
Liang Xiang,
Zixuan Song,
Shibo Xu,
Ke Wang,
Jiachen Chen,
Feitong Jin,
Xuhao Zhu,
Yu Gao,
Yaozu Wu,
Chuanyu Zhang,
Ning Wang,
Yiren Zou,
Ziqi Tan,
Aosai Zhang,
Zhengyi Cui,
Fanhao Shen,
Jiarun Zhong,
Tingting Li,
Jinfeng Deng,
Xu Zhang,
Hang Dong,
Pengfei Zhang
, et al. (8 additional authors not shown)
Abstract:
Tracking the time evolution of a quantum state allows one to verify the thermalization rate or the propagation speed of correlations in generic quantum systems. Inspired by the energy-time uncertainty principle, bounds have been demonstrated on the maximal speed at which a quantum state can change, resulting in immediate and practical tasks. Based on a programmable superconducting quantum processo…
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Tracking the time evolution of a quantum state allows one to verify the thermalization rate or the propagation speed of correlations in generic quantum systems. Inspired by the energy-time uncertainty principle, bounds have been demonstrated on the maximal speed at which a quantum state can change, resulting in immediate and practical tasks. Based on a programmable superconducting quantum processor, we test the dynamics of various emulated quantum mechanical systems encompassing single- and many-body states. We show that one can test the known quantum speed limits and that modifying a single Hamiltonian parameter allows the observation of the crossover of the different bounds on the dynamics. We also unveil the observation of minimal quantum speed limits in addition to more common maximal ones, i.e., the lowest rate of change of a unitarily evolved quantum state. Our results establish a comprehensive experimental characterization of quantum speed limits and pave the way for their subsequent study in engineered non-unitary conditions.
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Submitted 21 August, 2024;
originally announced August 2024.
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Petz map recovery for long-range entangled quantum many-body states
Authors:
Yangrui Hu,
Yijian Zou
Abstract:
Given a tripartite quantum state on $A,B,C$ and the erasure channel on $C$, the rotated Petz map is a recovery channel that acts on $B$ to recover the erased quantum information. The infidelity of the best recovery is upper-bounded by the conditional mutual information (CMI). In this work, we study the infidelity of the rotated Petz map on several physically-relevant long-range entangled quantum s…
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Given a tripartite quantum state on $A,B,C$ and the erasure channel on $C$, the rotated Petz map is a recovery channel that acts on $B$ to recover the erased quantum information. The infidelity of the best recovery is upper-bounded by the conditional mutual information (CMI). In this work, we study the infidelity of the rotated Petz map on several physically-relevant long-range entangled quantum states. Specifically, we study three classes of quantum phases: (i) steady states of measurement-induced phase transitions, (ii) critical ground state under local measurements, and (iii) chiral states under local measurements. We find that the averaged infidelity of the Petz map recovery sharply distinguishes the three classes: (i) and (ii) are distinguished by the scaling of the infidelity with CMI and (iii) is characterized by an asymmetry of the infidelity with the rotation parameter. We also study Petz map recovery for topological order and find an operational interpretation of the topological entanglement entropy. Our result indicates that recovery fidelity of the Petz map is a useful diagnostic of quantum phases of matter.
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Submitted 14 October, 2024; v1 submitted 1 August, 2024;
originally announced August 2024.
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Improved Nonlocality Certification via Bouncing between Bell Operators and Inequalities
Authors:
Weikang Li,
Mengyao Hu,
Ke Wang,
Shibo Xu,
Zhide Lu,
Jiachen Chen,
Yaozu Wu,
Chuanyu Zhang,
Feitong Jin,
Xuhao Zhu,
Yu Gao,
Zhengyi Cui,
Aosai Zhang,
Ning Wang,
Yiren Zou,
Fanhao Shen,
Jiarun Zhong,
Zehang Bao,
Zitian Zhu,
Pengfei Zhang,
Hekang Li,
Qiujiang Guo,
Zhen Wang,
Dong-Ling Deng,
Chao Song
, et al. (3 additional authors not shown)
Abstract:
Bell nonlocality is an intrinsic feature of quantum mechanics, which can be certified via the violation of Bell inequalities. It is therefore a fundamental question to certify Bell nonlocality from experimental data. Here, we present an optimization scheme to improve nonlocality certification by exploring flexible mappings between Bell inequalities and Hamiltonians corresponding to the Bell operat…
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Bell nonlocality is an intrinsic feature of quantum mechanics, which can be certified via the violation of Bell inequalities. It is therefore a fundamental question to certify Bell nonlocality from experimental data. Here, we present an optimization scheme to improve nonlocality certification by exploring flexible mappings between Bell inequalities and Hamiltonians corresponding to the Bell operators. We show that several Hamiltonian models can be mapped to new inequalities with improved classical bounds than the original one, enabling a more robust detection of nonlocality. From the other direction, we investigate the mapping from fixed Bell inequalities to Hamiltonians, aiming to maximize quantum violations while considering experimental imperfections. As a practical demonstration, we apply this method to an XXZ-like honeycomb-lattice model utilizing over 70 superconducting qubits. The successful application of this technique, as well as combining the two directions to form an optimization loop, may open new avenues for developing more practical and noise-resilient nonlocality certification techniques and enable broader experimental explorations.
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Submitted 17 July, 2024;
originally announced July 2024.
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Probing many-body Bell correlation depth with superconducting qubits
Authors:
Ke Wang,
Weikang Li,
Shibo Xu,
Mengyao Hu,
Jiachen Chen,
Yaozu Wu,
Chuanyu Zhang,
Feitong Jin,
Xuhao Zhu,
Yu Gao,
Ziqi Tan,
Aosai Zhang,
Ning Wang,
Yiren Zou,
Tingting Li,
Fanhao Shen,
Jiarun Zhong,
Zehang Bao,
Zitian Zhu,
Zixuan Song,
Jinfeng Deng,
Hang Dong,
Xu Zhang,
Pengfei Zhang,
Wenjie Jiang
, et al. (10 additional authors not shown)
Abstract:
Quantum nonlocality describes a stronger form of quantum correlation than that of entanglement. It refutes Einstein's belief of local realism and is among the most distinctive and enigmatic features of quantum mechanics. It is a crucial resource for achieving quantum advantages in a variety of practical applications, ranging from cryptography and certified random number generation via self-testing…
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Quantum nonlocality describes a stronger form of quantum correlation than that of entanglement. It refutes Einstein's belief of local realism and is among the most distinctive and enigmatic features of quantum mechanics. It is a crucial resource for achieving quantum advantages in a variety of practical applications, ranging from cryptography and certified random number generation via self-testing to machine learning. Nevertheless, the detection of nonlocality, especially in quantum many-body systems, is notoriously challenging. Here, we report an experimental certification of genuine multipartite Bell correlations, which signal nonlocality in quantum many-body systems, up to 24 qubits with a fully programmable superconducting quantum processor. In particular, we employ energy as a Bell correlation witness and variationally decrease the energy of a many-body system across a hierarchy of thresholds, below which an increasing Bell correlation depth can be certified from experimental data. As an illustrating example, we variationally prepare the low-energy state of a two-dimensional honeycomb model with 73 qubits and certify its Bell correlations by measuring an energy that surpasses the corresponding classical bound with up to 48 standard deviations. In addition, we variationally prepare a sequence of low-energy states and certify their genuine multipartite Bell correlations up to 24 qubits via energies measured efficiently by parity oscillation and multiple quantum coherence techniques. Our results establish a viable approach for preparing and certifying multipartite Bell correlations, which provide not only a finer benchmark beyond entanglement for quantum devices, but also a valuable guide towards exploiting multipartite Bell correlation in a wide spectrum of practical applications.
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Submitted 25 June, 2024;
originally announced June 2024.
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Approximate quantum error correcting codes from conformal field theory
Authors:
Shengqi Sang,
Timothy H. Hsieh,
Yijian Zou
Abstract:
The low-energy subspace of a conformal field theory (CFT) can serve as a quantum error correcting code, with important consequences in holography and quantum gravity. We consider generic 1+1D CFT codes under extensive local dephasing channels and analyze their error correctability in the thermodynamic limit. We show that (i) there is a finite decoding threshold if and only if the minimal nonzero s…
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The low-energy subspace of a conformal field theory (CFT) can serve as a quantum error correcting code, with important consequences in holography and quantum gravity. We consider generic 1+1D CFT codes under extensive local dephasing channels and analyze their error correctability in the thermodynamic limit. We show that (i) there is a finite decoding threshold if and only if the minimal nonzero scaling dimension in the fusion algebra generated by the jump operator of the channel is larger than $1/2$ and (ii) the number of protected logical qubits $k \geq Ω( \log \log n)$, where $n$ is the number of physical qubits. As an application, we show that the one-dimensional quantum critical Ising model has a finite threshold for certain types of dephasing noise. Our general results also imply that a CFT code with continuous symmetry saturates a bound on the recovery fidelity for covariant codes.
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Submitted 9 November, 2024; v1 submitted 13 June, 2024;
originally announced June 2024.
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Simulating unsteady fluid flows on a superconducting quantum processor
Authors:
Zhaoyuan Meng,
Jiarun Zhong,
Shibo Xu,
Ke Wang,
Jiachen Chen,
Feitong Jin,
Xuhao Zhu,
Yu Gao,
Yaozu Wu,
Chuanyu Zhang,
Ning Wang,
Yiren Zou,
Aosai Zhang,
Zhengyi Cui,
Fanhao Shen,
Zehang Bao,
Zitian Zhu,
Ziqi Tan,
Tingting Li,
Pengfei Zhang,
Shiying Xiong,
Hekang Li,
Qiujiang Guo,
Zhen Wang,
Chao Song
, et al. (2 additional authors not shown)
Abstract:
Recent advancements of intermediate-scale quantum processors have triggered tremendous interest in the exploration of practical quantum advantage. The simulation of fluid dynamics, a highly challenging problem in classical physics but vital for practical applications, emerges as a good candidate for showing quantum utility. Here, we report an experiment on the digital simulation of unsteady flows,…
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Recent advancements of intermediate-scale quantum processors have triggered tremendous interest in the exploration of practical quantum advantage. The simulation of fluid dynamics, a highly challenging problem in classical physics but vital for practical applications, emerges as a good candidate for showing quantum utility. Here, we report an experiment on the digital simulation of unsteady flows, which consists of quantum encoding, evolution, and detection of flow states, with a superconducting quantum processor. The quantum algorithm is based on the Hamiltonian simulation using the hydrodynamic formulation of the Schrödinger equation. With the median fidelities of 99.97% and 99.67% for parallel single- and two-qubit gates respectively, we simulate the dynamics of a two-dimensional (2D) compressible diverging flow and a 2D decaying vortex with ten qubits. The experimental results well capture the temporal evolution of averaged density and momentum profiles, and qualitatively reproduce spatial flow fields with moderate noises. This work demonstrates the potential of quantum computing in simulating more complex flows, such as turbulence, for practical applications.
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Submitted 24 April, 2024;
originally announced April 2024.
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Non-Abelian braiding of Fibonacci anyons with a superconducting processor
Authors:
Shibo Xu,
Zheng-Zhi Sun,
Ke Wang,
Hekang Li,
Zitian Zhu,
Hang Dong,
Jinfeng Deng,
Xu Zhang,
Jiachen Chen,
Yaozu Wu,
Chuanyu Zhang,
Feitong Jin,
Xuhao Zhu,
Yu Gao,
Aosai Zhang,
Ning Wang,
Yiren Zou,
Ziqi Tan,
Fanhao Shen,
Jiarun Zhong,
Zehang Bao,
Weikang Li,
Wenjie Jiang,
Li-Wei Yu,
Zixuan Song
, et al. (7 additional authors not shown)
Abstract:
Non-Abelian topological orders offer an intriguing path towards fault-tolerant quantum computation, where information can be encoded and manipulated in a topologically protected manner immune to arbitrary local noises and perturbations. However, realizing non-Abelian topologically ordered states is notoriously challenging in both condensed matter and programmable quantum systems, and it was not un…
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Non-Abelian topological orders offer an intriguing path towards fault-tolerant quantum computation, where information can be encoded and manipulated in a topologically protected manner immune to arbitrary local noises and perturbations. However, realizing non-Abelian topologically ordered states is notoriously challenging in both condensed matter and programmable quantum systems, and it was not until recently that signatures of non-Abelian statistics were observed through digital quantum simulation approaches. Despite these exciting progresses, none of them has demonstrated the appropriate type of topological orders and associated non-Abelian anyons whose braidings alone support universal quantum computation. Here, we report the realization of non-Abelian topologically ordered states of the Fibonacci string-net model and demonstrate braidings of Fibonacci anyons featuring universal computational power, with a superconducting quantum processor. We exploit efficient quantum circuits to prepare the desired states and verify their nontrivial topological nature by measuring the topological entanglement entropy. In addition, we create two pairs of Fibonacci anyons and demonstrate their fusion rule and non-Abelian braiding statistics by applying unitary gates on the underlying physical qubits. Our results establish a versatile digital approach to exploring exotic non-Abelian topological states and their associated braiding statistics with current noisy intermediate-scale quantum processors.
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Submitted 29 March, 2024;
originally announced April 2024.
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Measuring Spectral Form Factor in Many-Body Chaotic and Localized Phases of Quantum Processors
Authors:
Hang Dong,
Pengfei Zhang,
Ceren B. Dag,
Yu Gao,
Ning Wang,
Jinfeng Deng,
Xu Zhang,
Jiachen Chen,
Shibo Xu,
Ke Wang,
Yaozu Wu,
Chuanyu Zhang,
Feitong Jin,
Xuhao Zhu,
Aosai Zhang,
Yiren Zou,
Ziqi Tan,
Zhengyi Cui,
Zitian Zhu,
Fanhao Shen,
Tingting Li,
Jiarun Zhong,
Zehang Bao,
Hekang Li,
Zhen Wang
, et al. (6 additional authors not shown)
Abstract:
The spectral form factor (SFF) captures universal spectral fluctuations as signatures of quantum chaos, and has been instrumental in advancing multiple frontiers of physics including the studies of black holes and quantum many-body systems. However, the measurement of SFF in many-body systems is challenging due to the difficulty in resolving level spacings that become exponentially small with incr…
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The spectral form factor (SFF) captures universal spectral fluctuations as signatures of quantum chaos, and has been instrumental in advancing multiple frontiers of physics including the studies of black holes and quantum many-body systems. However, the measurement of SFF in many-body systems is challenging due to the difficulty in resolving level spacings that become exponentially small with increasing system size. Here we experimentally measure the SFF to probe the presence or absence of chaos in quantum many-body systems using a superconducting quantum processor with a randomized measurement protocol. For a Floquet chaotic system, we observe signatures of spectral rigidity of random matrix theory in SFF given by the ramp-plateau behavior. For a Hamiltonian system, we utilize SFF to distinguish the quantum many-body chaotic phase and the prethermal many-body localization. We observe the dip-ramp-plateau behavior of random matrix theory in the chaotic phase, and contrast the scaling of the plateau time in system size between the many-body chaotic and localized phases. Furthermore, we probe the eigenstate statistics by measuring a generalization of the SFF, known as the partial SFF, and observe distinct behaviors in the purities of the reduced density matrix in the two phases. This work unveils a new way of extracting the universal signatures of many-body quantum chaos in quantum devices by probing the correlations in eigenenergies and eigenstates.
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Submitted 25 March, 2024;
originally announced March 2024.
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Enhanced quantum state transfer: Circumventing quantum chaotic behavior
Authors:
Liang Xiang,
Jiachen Chen,
Zitian Zhu,
Zixuan Song,
Zehang Bao,
Xuhao Zhu,
Feitong Jin,
Ke Wang,
Shibo Xu,
Yiren Zou,
Hekang Li,
Zhen Wang,
Chao Song,
Alexander Yue,
Justine Partridge,
Qiujiang Guo,
Rubem Mondaini,
H. Wang,
Richard T. Scalettar
Abstract:
The ability to realize high-fidelity quantum communication is one of the many facets required to build generic quantum computing devices. In addition to quantum processing, sensing, and storage, transferring the resulting quantum states demands a careful design that finds no parallel in classical communication. Existing experimental demonstrations of quantum information transfer in solid-state qua…
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The ability to realize high-fidelity quantum communication is one of the many facets required to build generic quantum computing devices. In addition to quantum processing, sensing, and storage, transferring the resulting quantum states demands a careful design that finds no parallel in classical communication. Existing experimental demonstrations of quantum information transfer in solid-state quantum systems are largely confined to small chains with few qubits, often relying upon non-generic schemes. Here, by using a large-scale superconducting quantum circuit featuring thirty-six tunable qubits, accompanied by general optimization procedures deeply rooted in overcoming quantum chaotic behavior, we demonstrate a scalable protocol for transferring few-particle quantum states in a two-dimensional quantum network. These include single-qubit excitation and also two-qubit entangled states, and two excitations for which many-body effects are present. Our approach, combined with the quantum circuit's versatility, paves the way to short-distance quantum communication for connecting distributed quantum processors or registers, even if hampered by inherent imperfections in actual quantum devices.
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Submitted 1 February, 2024;
originally announced February 2024.
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Creating and controlling global Greenberger-Horne-Zeilinger entanglement on quantum processors
Authors:
Zehang Bao,
Shibo Xu,
Zixuan Song,
Ke Wang,
Liang Xiang,
Zitian Zhu,
Jiachen Chen,
Feitong Jin,
Xuhao Zhu,
Yu Gao,
Yaozu Wu,
Chuanyu Zhang,
Ning Wang,
Yiren Zou,
Ziqi Tan,
Aosai Zhang,
Zhengyi Cui,
Fanhao Shen,
Jiarun Zhong,
Tingting Li,
Jinfeng Deng,
Xu Zhang,
Hang Dong,
Pengfei Zhang,
Yang-Ren Liu
, et al. (8 additional authors not shown)
Abstract:
Greenberger-Horne-Zeilinger (GHZ) states, also known as two-component Schrödinger cats, play vital roles in the foundation of quantum physics and, more attractively, in future quantum technologies such as fault-tolerant quantum computation. Enlargement in size and coherent control of GHZ states are both crucial for harnessing entanglement in advanced computational tasks with practical advantages,…
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Greenberger-Horne-Zeilinger (GHZ) states, also known as two-component Schrödinger cats, play vital roles in the foundation of quantum physics and, more attractively, in future quantum technologies such as fault-tolerant quantum computation. Enlargement in size and coherent control of GHZ states are both crucial for harnessing entanglement in advanced computational tasks with practical advantages, which unfortunately pose tremendous challenges as GHZ states are vulnerable to noise. Here we propose a general strategy for creating, preserving, and manipulating large-scale GHZ entanglement, and demonstrate a series of experiments underlined by high-fidelity digital quantum circuits. For initialization, we employ a scalable protocol to create genuinely entangled GHZ states with up to 60 qubits, almost doubling the previous size record. For protection, we take a new perspective on discrete time crystals (DTCs), originally for exploring exotic nonequilibrium quantum matters, and embed a GHZ state into the eigenstates of a tailor-made cat scar DTC to extend its lifetime. For manipulation, we switch the DTC eigenstates with in-situ quantum gates to modify the effectiveness of the GHZ protection. Our findings establish a viable path towards coherent operations on large-scale entanglement, and further highlight superconducting processors as a promising platform to explore nonequilibrium quantum matters and emerging applications.
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Submitted 13 October, 2024; v1 submitted 16 January, 2024;
originally announced January 2024.
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Long-lived topological time-crystalline order on a quantum processor
Authors:
Liang Xiang,
Wenjie Jiang,
Zehang Bao,
Zixuan Song,
Shibo Xu,
Ke Wang,
Jiachen Chen,
Feitong Jin,
Xuhao Zhu,
Zitian Zhu,
Fanhao Shen,
Ning Wang,
Chuanyu Zhang,
Yaozu Wu,
Yiren Zou,
Jiarun Zhong,
Zhengyi Cui,
Aosai Zhang,
Ziqi Tan,
Tingting Li,
Yu Gao,
Jinfeng Deng,
Xu Zhang,
Hang Dong,
Pengfei Zhang
, et al. (16 additional authors not shown)
Abstract:
Topologically ordered phases of matter elude Landau's symmetry-breaking theory, featuring a variety of intriguing properties such as long-range entanglement and intrinsic robustness against local perturbations. Their extension to periodically driven systems gives rise to exotic new phenomena that are forbidden in thermal equilibrium. Here, we report the observation of signatures of such a phenomen…
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Topologically ordered phases of matter elude Landau's symmetry-breaking theory, featuring a variety of intriguing properties such as long-range entanglement and intrinsic robustness against local perturbations. Their extension to periodically driven systems gives rise to exotic new phenomena that are forbidden in thermal equilibrium. Here, we report the observation of signatures of such a phenomenon -- a prethermal topologically ordered time crystal -- with programmable superconducting qubits arranged on a square lattice. By periodically driving the superconducting qubits with a surface-code Hamiltonian, we observe discrete time-translation symmetry breaking dynamics that is only manifested in the subharmonic temporal response of nonlocal logical operators. We further connect the observed dynamics to the underlying topological order by measuring a nonzero topological entanglement entropy and studying its subsequent dynamics. Our results demonstrate the potential to explore exotic topologically ordered nonequilibrium phases of matter with noisy intermediate-scale quantum processors.
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Submitted 8 January, 2024;
originally announced January 2024.
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Disorder-tunable entanglement at infinite temperature
Authors:
Hang Dong,
Jean-Yves Desaules,
Yu Gao,
Ning Wang,
Zexian Guo,
Jiachen Chen,
Yiren Zou,
Feitong Jin,
Xuhao Zhu,
Pengfei Zhang,
Hekang Li,
Zhen Wang,
Qiujiang Guo,
Junxiang Zhang,
Lei Ying,
Zlatko Papić
Abstract:
Emerging quantum technologies hold the promise of unraveling difficult problems ranging from condensed matter to high energy physics, while at the same time motivating the search for unprecedented phenomena in their setting. Here we utilize a custom-built superconducting qubit ladder to realize non-thermalizing states with rich entanglement structures in the middle of the energy spectrum. Despite…
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Emerging quantum technologies hold the promise of unraveling difficult problems ranging from condensed matter to high energy physics, while at the same time motivating the search for unprecedented phenomena in their setting. Here we utilize a custom-built superconducting qubit ladder to realize non-thermalizing states with rich entanglement structures in the middle of the energy spectrum. Despite effectively forming an "infinite" temperature ensemble, these states robustly encode quantum information far from equilibrium, as we demonstrate by measuring the fidelity and entanglement entropy in the quench dynamics of the ladder. Our approach harnesses the recently proposed type of non-ergodic behavior known as "rainbow scar", which allows us to obtain analytically exact eigenfunctions whose ergodicity-breaking properties can be conveniently controlled by randomizing the couplings of the model, without affecting their energy. The on-demand tunability of quantum correlations via disorder allows for in situ control over ergodicity breaking and it provides a knob for designing exotic many-body states that defy thermalization.
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Submitted 3 September, 2024; v1 submitted 15 December, 2023;
originally announced December 2023.
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Dynamical relaxation of a long-range XY chain
Authors:
Yu-Huang Huang,
Yin-Tao Zou,
Chengxiang Ding
Abstract:
We study the universal real-time relaxation behaviors of a long-range quantum XY chain following a quench. Our research includes both the noncritical and critical quench. In the case of noncritical quench, i.e., neither the initial state nor the postquench Hamiltonian is at a critical point of equilibrium phase transition, a quench to the commensurate phase or incommensurate phase gives a scaling…
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We study the universal real-time relaxation behaviors of a long-range quantum XY chain following a quench. Our research includes both the noncritical and critical quench. In the case of noncritical quench, i.e., neither the initial state nor the postquench Hamiltonian is at a critical point of equilibrium phase transition, a quench to the commensurate phase or incommensurate phase gives a scaling of $t^{-3/2}$ or $t^{-1/2}$, respectively, which is the same as the counterpart of the short-range XY model. However, for a quench to the boundary line between the commensurate and incommensurate phases, the scaling law $t^{-μ}$ may be different from the $t^{-3/4}$ law of the counterpart of the short-range model. More interestingly, the decaying exponent $μ$ may depend on the choice of the parameters of the postquench Hamiltonian because of the different asymptotic behaviors of the energy spectrum. Furthermore, in certain cases, the scaling behavior may be outside the range of predictions made by the stationary phase approximation, because an inflection point emerges in the energy spectrum. For the critical quench, i.e., the initial state or the postquench Hamiltonian is at a critical point of equilibrium phase transition, the aforementioned scaling law $t^{-μ}$ may be changed because of the gap-closing property of the energy spectrum of the critical point.
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Submitted 3 December, 2023; v1 submitted 30 November, 2023;
originally announced November 2023.
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Mixed-state Quantum Phases: Renormalization and Quantum Error Correction
Authors:
Shengqi Sang,
Yijian Zou,
Timothy H. Hsieh
Abstract:
Open system quantum dynamics can generate a variety of long-range entangled mixed states, yet it has been unclear in what sense they constitute phases of matter. To establish that two mixed states are in the same phase, as defined by their two-way connectivity via local quantum channels, we use the renormalization group (RG) and decoders of quantum error correcting codes. We introduce a real-space…
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Open system quantum dynamics can generate a variety of long-range entangled mixed states, yet it has been unclear in what sense they constitute phases of matter. To establish that two mixed states are in the same phase, as defined by their two-way connectivity via local quantum channels, we use the renormalization group (RG) and decoders of quantum error correcting codes. We introduce a real-space RG scheme for mixed states based on local channels which ideally preserve correlations with the complementary system, and we prove this is equivalent to the reversibility of the channel's action. As an application, we demonstrate an exact RG flow of finite temperature toric code in two dimensions to infinite temperature, thus proving it is in the trivial phase. In contrast, for toric code subject to local dephasing, we establish a mixed state toric code phase using local channels obtained by truncating an RG-type decoder and the minimum weight perfect matching decoder. We also discover a precise relation between mixed state phase and decodability, by proving that local noise acting on toric code cannot destroy logical information without bringing the state out of the toric code phase.
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Submitted 25 February, 2026; v1 submitted 12 October, 2023;
originally announced October 2023.
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Petz recovery from subsystems in conformal field theory
Authors:
Shreya Vardhan,
Annie Y. Wei,
Yijian Zou
Abstract:
We probe the multipartite entanglement structure of the vacuum state of a CFT in 1+1 dimensions, using recovery operations that attempt to reconstruct the density matrix in some region from its reduced density matrices on smaller subregions. We use an explicit recovery channel known as the twirled Petz map, and study distance measures such as the fidelity, relative entropy, and trace distance betw…
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We probe the multipartite entanglement structure of the vacuum state of a CFT in 1+1 dimensions, using recovery operations that attempt to reconstruct the density matrix in some region from its reduced density matrices on smaller subregions. We use an explicit recovery channel known as the twirled Petz map, and study distance measures such as the fidelity, relative entropy, and trace distance between the original state and the recovered state. One setup we study in detail involves three contiguous intervals $A$, $B$ and $C$ on a spatial slice, where we can view these quantities as measuring correlations between $A$ and $C$ that are not mediated by the region $B$ that lies between them. We show that each of the distance measures is both UV finite and independent of the operator content of the CFT, and hence depends only on the central charge and the cross-ratio of the intervals. We evaluate these universal quantities numerically using lattice simulations in critical spin chain models, and derive their analytic forms in the limit where $A$ and $C$ are close using the OPE expansion. In the case where $A$ and $C$ are far apart, we find a surprising non-commutativity of the replica trick with the OPE limit. For all values of the cross-ratio, the fidelity is strictly better than a general information-theoretic lower bound in terms of the conditional mutual information. We also compare the mutual information between various subsystems in the original and recovered states, which leads to a more qualitative understanding of the differences between them. Further, we introduce generalizations of the recovery operation to more than three adjacent intervals, for which the fidelity is again universal with respect to the operator content.
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Submitted 26 July, 2023;
originally announced July 2023.
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The Role of Nonequilibrium LO Phonons, Pauli Exclusion, and Intervalley Pathways on the Relaxation of Hot Carriers in InGaAs Multi-Quantum-Well Structures
Authors:
Yongjie Zou,
Hamidreza Esmaielpour,
Daniel Suchet,
Jean-François Guillemoles,
Stephen M. Goodnick
Abstract:
Under continuous-wave laser excitation in an InGaAs multi-quantum-well (MQW) structure, the carrier temperature extracted from photoluminescence rises faster for 405 nm excitation compared with 980 nm excitation, as the injected carrier density increases. Ensemble Monte Carlo simulation of the carrier dynamics in the MQW system shows that this carrier temperature rise is dominated by nonequilibriu…
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Under continuous-wave laser excitation in an InGaAs multi-quantum-well (MQW) structure, the carrier temperature extracted from photoluminescence rises faster for 405 nm excitation compared with 980 nm excitation, as the injected carrier density increases. Ensemble Monte Carlo simulation of the carrier dynamics in the MQW system shows that this carrier temperature rise is dominated by nonequilibrium LO phonon effects, with the Pauli exclusion having a significant effect at high carrier densities. Further, we find a significant fraction of carriers reside in the satellite L-valleys for 405 nm excitation due to strong intervalley transfer, leading to a cooler steady-state electron temperature in the central valley compared with the case when intervalley transfer is excluded from the model. Good agreement between experiment and simulation has been shown, and a detailed analysis has been presented. This study expands our knowledge of the dynamics of the hot carrier population in semiconductors, which can be applied to further limit energy loss in solar cells.
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Submitted 6 March, 2023;
originally announced March 2023.
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Channeling quantum criticality
Authors:
Yijian Zou,
Shengqi Sang,
Timothy H. Hsieh
Abstract:
We analyze the effect of decoherence, modelled by local quantum channels, on quantum critical states and we find universal properties of the resulting mixed state's entanglement, both between system and environment and within the system. Renyi entropies exhibit volume law scaling with a subleading constant governed by a "$g$-function" in conformal field theory (CFT), allowing us to define a notion…
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We analyze the effect of decoherence, modelled by local quantum channels, on quantum critical states and we find universal properties of the resulting mixed state's entanglement, both between system and environment and within the system. Renyi entropies exhibit volume law scaling with a subleading constant governed by a "$g$-function" in conformal field theory (CFT), allowing us to define a notion of renormalization group (RG) flow (or "phase transitions") between quantum channels. We also find that the entropy of a subsystem in the decohered state has a subleading logarithmic scaling with subsystem size, and we relate it to correlation functions of boundary condition changing operators in the CFT. Finally, we find that the subsystem entanglement negativity, a measure of quantum correlations within mixed states, can exhibit log scaling or area law based on the RG flow. When the channel corresponds to a marginal perturbation, the coefficient of the log scaling can change continuously with decoherence strength. We illustrate all these possibilities for the critical ground state of the transverse-field Ising model, in which we identify four RG fixed points of dephasing channels and verify the RG flow numerically. Our results are relevant to quantum critical states realized on noisy quantum simulators, in which our predicted entanglement scaling can be probed via shadow tomography methods.
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Submitted 22 June, 2023; v1 submitted 17 January, 2023;
originally announced January 2023.
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Digital simulation of non-Abelian anyons with 68 programmable superconducting qubits
Authors:
Shibo Xu,
Zheng-Zhi Sun,
Ke Wang,
Liang Xiang,
Zehang Bao,
Zitian Zhu,
Fanhao Shen,
Zixuan Song,
Pengfei Zhang,
Wenhui Ren,
Xu Zhang,
Hang Dong,
Jinfeng Deng,
Jiachen Chen,
Yaozu Wu,
Ziqi Tan,
Yu Gao,
Feitong Jin,
Xuhao Zhu,
Chuanyu Zhang,
Ning Wang,
Yiren Zou,
Jiarun Zhong,
Aosai Zhang,
Weikang Li
, et al. (9 additional authors not shown)
Abstract:
Non-Abelian anyons are exotic quasiparticle excitations hosted by certain topological phases of matter. They break the fermion-boson dichotomy and obey non-Abelian braiding statistics: their interchanges yield unitary operations, rather than merely a phase factor, in a space spanned by topologically degenerate wavefunctions. They are the building blocks of topological quantum computing. However, e…
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Non-Abelian anyons are exotic quasiparticle excitations hosted by certain topological phases of matter. They break the fermion-boson dichotomy and obey non-Abelian braiding statistics: their interchanges yield unitary operations, rather than merely a phase factor, in a space spanned by topologically degenerate wavefunctions. They are the building blocks of topological quantum computing. However, experimental observation of non-Abelian anyons and their characterizing braiding statistics is notoriously challenging and has remained elusive hitherto, in spite of various theoretical proposals. Here, we report an experimental quantum digital simulation of projective non-Abelian anyons and their braiding statistics with up to 68 programmable superconducting qubits arranged on a two-dimensional lattice. By implementing the ground states of the toric-code model with twists through quantum circuits, we demonstrate that twists exchange electric and magnetic charges and behave as a particular type of non-Abelian anyons, i.e., the Ising anyons. In particular, we show experimentally that these twists follow the fusion rules and non-Abelian braiding statistics of the Ising type, and can be explored to encode topological logical qubits. Furthermore, we demonstrate how to implement both single- and two-qubit logic gates through applying a sequence of elementary Pauli gates on the underlying physical qubits. Our results demonstrate a versatile quantum digital approach for simulating non-Abelian anyons, offering a new lens into the study of such peculiar quasiparticles.
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Submitted 11 May, 2023; v1 submitted 17 November, 2022;
originally announced November 2022.
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Observation of many-body Fock space dynamics in two dimensions
Authors:
Yunyan Yao,
Liang Xiang,
Zexian Guo,
Zehang Bao,
Yong-Feng Yang,
Zixuan Song,
Haohai Shi,
Xuhao Zhu,
Feitong Jin,
Jiachen Chen,
Shibo Xu,
Zitian Zhu,
Fanhao Shen,
Ning Wang,
Chuanyu Zhang,
Yaozu Wu,
Yiren Zou,
Pengfei Zhang,
Hekang Li,
Zhen Wang,
Chao Song,
Chen Cheng,
Rubem Mondaini,
H. Wang,
J. Q. You
, et al. (3 additional authors not shown)
Abstract:
Quantum many-body simulation provides a straightforward way to understand fundamental physics and connect with quantum information applications. However, suffering from exponentially growing Hilbert space size, characterization in terms of few-body probes in real space is often insufficient to tackle challenging problems such as quantum critical behavior and many-body localization (MBL) in higher…
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Quantum many-body simulation provides a straightforward way to understand fundamental physics and connect with quantum information applications. However, suffering from exponentially growing Hilbert space size, characterization in terms of few-body probes in real space is often insufficient to tackle challenging problems such as quantum critical behavior and many-body localization (MBL) in higher dimensions. Here, we experimentally employ a new paradigm on a superconducting quantum processor, exploring such elusive questions from a Fock space view: mapping the many-body system onto an unconventional Anderson model on a complex Fock space network of many-body states. By observing the wave packet propagating in Fock space and the emergence of a statistical ergodic ensemble, we reveal a fresh picture for characterizing representative many-body dynamics: thermalization, localization, and scarring. In addition, we observe a quantum critical regime of anomalously enhanced wave packet width and deduce a critical point from the maximum wave packet fluctuations, which lend support for the two-dimensional MBL transition in finite-sized systems. Our work unveils a new perspective of exploring many-body physics in Fock space, demonstrating its practical applications on contentious MBL aspects such as criticality and dimensionality. Moreover, the entire protocol is universal and scalable, paving the way to finally solve a broader range of controversial many-body problems on future larger quantum devices.
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Submitted 10 November, 2022;
originally announced November 2022.
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Cross Entropy Benchmark for Measurement-Induced Phase Transitions
Authors:
Yaodong Li,
Yijian Zou,
Paolo Glorioso,
Ehud Altman,
Matthew P. A. Fisher
Abstract:
We investigate the prospects of employing the linear cross-entropy to experimentally access measurement-induced phase transitions (MIPT) without requiring any postselection of quantum trajectories. For two random circuits that are identical in the bulk but with different initial states, the linear cross-entropy $χ$ between the bulk measurement outcome distributions in the two circuits acts as a bo…
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We investigate the prospects of employing the linear cross-entropy to experimentally access measurement-induced phase transitions (MIPT) without requiring any postselection of quantum trajectories. For two random circuits that are identical in the bulk but with different initial states, the linear cross-entropy $χ$ between the bulk measurement outcome distributions in the two circuits acts as a boundary order parameter, and can be used to distinguish the volume law from area law phases. In the volume law phase (and in the thermodynamic limit) the bulk measurements cannot distinguish between the two different initial states, and $χ= 1$. In the area law phase $χ< 1$. For circuits with Clifford gates, we provide numerical evidence that $χ$ can be sampled to accuracy $ε$ from $O(1/ε^2)$ trajectories, by running the first circuit on a quantum simulator without postselection, aided by a classical simulation of the second. We also find that for weak depolarizing noise the signature of the MIPT is still present for intermediate system sizes. In our protocol we have the freedom of choosing initial states such that the "classical" side can be simulated efficiently, while simulating the "quantum" side is still classically hard.
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Submitted 7 June, 2023; v1 submitted 1 September, 2022;
originally announced September 2022.
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Detecting bulk and edge exceptional points in non-Hermitian systems through generalized Petermann factors
Authors:
Yue-Yu Zou,
Yao Zhou,
Li-Mei Chen,
Peng Ye
Abstract:
Non-orthogonality in non-Hermitian quantum systems gives rise to tremendous exotic quantum phenomena, which can be fundamentally traced back to non-unitarity and is much more fundamental and universal than complex energy spectrum. In this paper, we introduce an interesting quantity (denoted as $η$) as a new variant of the Petermann factor to directly and efficiently measure non-unitarity and the a…
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Non-orthogonality in non-Hermitian quantum systems gives rise to tremendous exotic quantum phenomena, which can be fundamentally traced back to non-unitarity and is much more fundamental and universal than complex energy spectrum. In this paper, we introduce an interesting quantity (denoted as $η$) as a new variant of the Petermann factor to directly and efficiently measure non-unitarity and the associated non-Hermitian physics. By tuning the model parameters of underlying non-Hermitian systems, we find that the discontinuity of both $η$ and its first-order derivative (denoted as $\partial η$) pronouncedly captures rich physics that is fundamentally caused by non-unitarity. More concretely, in the 1D non-Hermitian topological systems, two mutually orthogonal edge states that are respectively localized on two boundaries become non-orthogonal in the vicinity of discontinuity of $η$ as a function of the model parameter, which is dubbed ``edge state transition''. Through theoretical analysis, we identify that the appearance of edge state transition indicates the existence of exceptional points~(EPs) in topological edge states. Regarding the discontinuity of $\partialη$, we investigate a two-level non-Hermitian model and establish a connection between the points of discontinuity of $\partial η$ and EPs of bulk states. By studying this connection in more general lattice models, we find that some models have discontinuity of $\partialη$, implying the existence of EPs in bulk states.
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Submitted 20 April, 2023; v1 submitted 31 August, 2022;
originally announced August 2022.
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Integrating a fiber cavity into a wheel trap for strong ion-cavity coupling
Authors:
Markus Teller,
Viktor Messerer,
Klemens Schüppert,
Yueyang Zou,
Dario A. Fioretto,
Maria Galli,
Philip C. Holz,
Jakob Reichel,
Tracy E. Northup
Abstract:
We present an ion trap with an integrated fiber cavity, designed for strong coupling at the level of single ions and photons. The cavity is aligned to the axis of a miniature linear Paul trap, enabling simultaneous coupling of multiple ions to the cavity field. We simulate how charges on the fiber mirrors affect the trap potential, and we test these predictions with an ion trapped in the cavity. F…
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We present an ion trap with an integrated fiber cavity, designed for strong coupling at the level of single ions and photons. The cavity is aligned to the axis of a miniature linear Paul trap, enabling simultaneous coupling of multiple ions to the cavity field. We simulate how charges on the fiber mirrors affect the trap potential, and we test these predictions with an ion trapped in the cavity. Furthermore, we measure micromotion and heating rates in the setup.
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Submitted 21 July, 2022;
originally announced July 2022.
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Emergence of Kac-Moody Symmetry in Critical Quantum Spin Chains
Authors:
Ruoshui Wang,
Yijian Zou,
Guifre Vidal
Abstract:
Given a critical quantum spin chain with a microscopic Lie-group symmetry, corresponding e.g. to $U(1)$ or $SU(2)$ spin isotropy, we numerically investigate the emergence of Kac-Moody symmetry at low energies and long distances. In that regime, one such critical quantum spin chain is described by a conformal field theory where the usual Virasoro algebra associated to conformal invariance is augmen…
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Given a critical quantum spin chain with a microscopic Lie-group symmetry, corresponding e.g. to $U(1)$ or $SU(2)$ spin isotropy, we numerically investigate the emergence of Kac-Moody symmetry at low energies and long distances. In that regime, one such critical quantum spin chain is described by a conformal field theory where the usual Virasoro algebra associated to conformal invariance is augmented with a Kac-Moody algebra associated to conserved currents. Specifically, we first propose a method to construct lattice operators corresponding to the Kac-Moody generators. We then numerically show that, when projected onto low energy states of the quantum spin chain, these operators indeed approximately fulfill the Kac-Moody algebra. The lattice version of the Kac-Moody generators allow us to compute the so-called level constant and to organize the low-energy eigenstates of the lattice Hamiltonian into Kac-Moody towers. We illustrate the proposal with the XXZ model and the Heisenberg model with a next-to-nearest-neighbor coupling.
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Submitted 3 June, 2022;
originally announced June 2022.
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Modular Commutators in Conformal Field Theory
Authors:
Yijian Zou,
Bowen Shi,
Jonathan Sorce,
Ian T. Lim,
Isaac H. Kim
Abstract:
The modular commutator is a recently discovered multipartite entanglement measure that quantifies the chirality of the underlying many-body quantum state. In this Letter, we derive a universal expression for the modular commutator in conformal field theories in $1+1$ dimensions and discuss its salient features. We show that the modular commutator depends only on the chiral central charge and the c…
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The modular commutator is a recently discovered multipartite entanglement measure that quantifies the chirality of the underlying many-body quantum state. In this Letter, we derive a universal expression for the modular commutator in conformal field theories in $1+1$ dimensions and discuss its salient features. We show that the modular commutator depends only on the chiral central charge and the conformal cross ratio. We test this formula for a gapped $(2+1)$-dimensional system with a chiral edge, i.e., the quantum Hall state, and observe excellent agreement with numerical simulations. Furthermore, we propose a geometric dual for the modular commutator in certain preferred states of the AdS/CFT correspondence. For these states, we argue that the modular commutator can be obtained from a set of crossing angles between intersecting Ryu-Takayanagi surfaces.
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Submitted 14 June, 2022; v1 submitted 31 May, 2022;
originally announced June 2022.
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Probing sign structure using measurement-induced entanglement
Authors:
Cheng-Ju Lin,
Weicheng Ye,
Yijian Zou,
Shengqi Sang,
Timothy H. Hsieh
Abstract:
The sign structure of quantum states is closely connected to quantum phases of matter, yet detecting such fine-grained properties of amplitudes is subtle. Here we employ as a diagnostic measurement-induced entanglement (MIE): the average entanglement generated between two parties after measuring the rest of the system. We propose that for a sign-free state, the MIE upon measuring in the sign-free…
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The sign structure of quantum states is closely connected to quantum phases of matter, yet detecting such fine-grained properties of amplitudes is subtle. Here we employ as a diagnostic measurement-induced entanglement (MIE): the average entanglement generated between two parties after measuring the rest of the system. We propose that for a sign-free state, the MIE upon measuring in the sign-free basis decays no slower than correlations in the state before measurement. Concretely, we prove that MIE is upper bounded by mutual information for sign-free stabilizer states (essentially CSS codes), which establishes a bound between scaling dimensions of conformal field theories describing measurement-induced critical points in stabilizer systems. We also show that for sign-free qubit wavefunctions, MIE between two qubits is upper bounded by a simple two-point correlation function, and we verify our proposal in several critical ground states of one-dimensional systems, including the transverse field and tri-critical Ising models. In contrast, for states with sign structure, such bounds can be violated, as we illustrate in critical hybrid circuits involving both Haar or Clifford random unitaries and measurements, and gapless symmetry-protected topological states.
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Submitted 24 January, 2023; v1 submitted 11 May, 2022;
originally announced May 2022.
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Glass-patternable notch-shaped microwave architecture for on-chip spin detection in biological samples
Authors:
Keisuke Oshimi,
Yushi Nishimura,
Tsutomu Matsubara,
Masuaki Tanaka,
Eiji Shikoh,
Li Zhao,
Yajuan Zou,
Naoki Komatsu,
Yuta Ikado,
Yuka Takezawa,
Eriko Kage-Nakadai,
Yumi Izutsu,
Katsutoshi Yoshizato,
Saho Morita,
Masato Tokunaga,
Hiroshi Yukawa,
Yoshinobu Baba,
Yoshio Teki,
Masazumi Fujiwara
Abstract:
We report a notch-shaped coplanar microwave waveguide antenna on a glass plate designed for on-chip detection of optically detected magnetic resonance (ODMR) of fluorescent nanodiamonds (NDs). A lithographically patterned thin wire at the center of the notch area in the coplanar waveguide realizes a millimeter-scale ODMR detection area (1.5 x 2.0 mm^2) and gigahertz-broadband characteristics with…
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We report a notch-shaped coplanar microwave waveguide antenna on a glass plate designed for on-chip detection of optically detected magnetic resonance (ODMR) of fluorescent nanodiamonds (NDs). A lithographically patterned thin wire at the center of the notch area in the coplanar waveguide realizes a millimeter-scale ODMR detection area (1.5 x 2.0 mm^2) and gigahertz-broadband characteristics with low reflection (about 8%). The ODMR signal intensity in the detection area is quantitatively predictable by numerical simulation. Using this chip device, we demonstrate a uniform ODMR signal intensity over the detection area for cells, tissue, and worms. The present demonstration of a chip-based microwave architecture will enable scalable chip integration of ODMR-based quantum sensing technology into various bioassay platforms.
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Submitted 5 May, 2022;
originally announced May 2022.
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Density Matrix Renormalization Group with Tensor Processing Units
Authors:
Martin Ganahl,
Jackson Beall,
Markus Hauru,
Adam G. M. Lewis,
Jae Hyeon Yoo,
Yijian Zou,
Guifre Vidal
Abstract:
Google's Tensor Processing Units (TPUs) are integrated circuits specifically built to accelerate and scale up machine learning workloads. They can perform fast distributed matrix multiplications and therefore be repurposed for other computationally intensive tasks. In this work we demonstrate the use of TPUs for accelerating and scaling up the density matrix renormalization group (DMRG), a powerfu…
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Google's Tensor Processing Units (TPUs) are integrated circuits specifically built to accelerate and scale up machine learning workloads. They can perform fast distributed matrix multiplications and therefore be repurposed for other computationally intensive tasks. In this work we demonstrate the use of TPUs for accelerating and scaling up the density matrix renormalization group (DMRG), a powerful numerical approach to compute the ground state of a local quantum many-body Hamiltonian. The cost of DMRG scales with system size $N$ as $O(ND^3)$, where the so-called bond dimension $D$ regulates how expressive the underlying matrix product state (MPS) variational ansatz is. We consider lattice models in two spatial dimensions, with square lattices of size $10\times 10$ (free fermions) and $20\times 20$ (transverse field Ising model), for which the required MPS bond dimension is known to scale at least as $\exp(\sqrt{N})$. Using half of a TPU v3 pod (namely $1,\!024$ TPU v3 cores) we reached an unprecedentedly large bond dimension $D = 2^{16} = 65,\!536$, for which optimizing a single MPS tensor took about 2 minutes.
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Submitted 12 April, 2022;
originally announced April 2022.
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Operator fusion from wavefunction overlaps: Universal finite-size corrections and application to Haagerup model
Authors:
Yuhan Liu,
Yijian Zou,
Shinsei Ryu
Abstract:
Given a critical quantum spin chain described by a conformal field theory (CFT) at long distances, it is crucial to understand the universal conformal data. One most important ingredient is the operator product expansion (OPE) coefficients, which describe how operators fuse into each other. It has been proposed in [Zou, Vidal, Phys. Rev. B 105, 125125] that the OPE coefficients can be computed fro…
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Given a critical quantum spin chain described by a conformal field theory (CFT) at long distances, it is crucial to understand the universal conformal data. One most important ingredient is the operator product expansion (OPE) coefficients, which describe how operators fuse into each other. It has been proposed in [Zou, Vidal, Phys. Rev. B 105, 125125] that the OPE coefficients can be computed from overlaps of low-energy wavefunctions of the spin chain. In this work, we establish that all conformal data including central charge, conformal dimensions, and OPE coefficients are encoded in the wavefunction overlaps, with universal finite-size corrections that depend on the operator content of the cyclic orbifold CFT. Thus this method allows us to numerically compute all the conformal data based solely on the low-energy eigenstates. The predictions are verified in the Ising and XXZ model. As an application, we study the recently proposed Haagerup model built from the Haagerup fusion category. We find that the CFT has central charge $c \approx 2.1$ and the lowest spin-$1$ operator in the twisted sector has scaling dimension $1 < Δ_J \leq 1.4$.
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Submitted 28 March, 2022;
originally announced March 2022.
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A universal tripartite entanglement signature of ungappable edge states
Authors:
Karthik Siva,
Yijian Zou,
Tomohiro Soejima,
Roger S. K. Mong,
Michael P. Zaletel
Abstract:
Gapped two-dimensional topological phases can feature ungappable edge states which are robust even in the absence of protecting symmetries. In this work we show that a multipartite entanglement measure recently proposed in the context of holography, the Markov gap, provides a universal diagnostic of ungappable edge states. Defined as a difference of the reflected entropy and mutual information…
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Gapped two-dimensional topological phases can feature ungappable edge states which are robust even in the absence of protecting symmetries. In this work we show that a multipartite entanglement measure recently proposed in the context of holography, the Markov gap, provides a universal diagnostic of ungappable edge states. Defined as a difference of the reflected entropy and mutual information $h(A:B) = S_R(A:B) - I(A:B)$ between two parties, we argue that for $A,B$ being adjacent subregions in the bulk, $h=\frac{c_+}{3}\log 2$, where $c_+$ is the minimal total central charge of the boundary theory. As evidence, we prove that $h=0$ for string-net models, and numerically verify that $h=\frac{|C|}{3}\log 2$ for a Chern-$C$ insulator. Our work establishes a unique bulk entanglement criteria for the presence of a conformal field theory on the boundary.
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Submitted 22 October, 2021;
originally announced October 2021.