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arXiv:2608.01111

Fault-tolerant quantum computing with a microwave Cat Bus

Yanyan Chen, Xinyang Yu, Yueyang Min, Zhihao Zhang, Shuaifan Cao, Xiaopeng Li

quant-phSubmitted Aug 2, 2026• Announced Aug 4, 2026• 0 citations
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Abstract

The scalability of fault-tolerant neutral-atom quantum computers is constrained by the latency of shuttling with optical tweezers, imposing a stringent trade-off between qubit overhead and circuit depth in quantum algorithm compilation. Here we propose a hardware-efficient, shuttling-free architecture that achieves all-to-all connectivity. Remote Rydberg atoms are resonantly entangled through a microwave ``Cat Bus''---a cavity mode autonomously stabilized in a bosonic cat state. The Cat Bus natively supports the highly parallelized execution of one-to-many $\mathrm{CZ}^n$ gates with exponentially suppressed crosstalk. We derive the resulting cat--atom error channel from the underlying interactions and physical constraints. For fault-tolerant operation, we develop a hardware-aware scheduling scheme that exploits the native cat--atom $\mathrm{CZ}^{n}$ gate to construct a syndrome-extraction circuit with minimum depth. We benchmark the architecture using hypergraph-product (HGP) codes and estimate a 180-fold reduction in syndrome-extraction cycle time at $N=10^5$ data qubits compared with an atom-rearrangement-based architecture. Under matched two-qubit depolarizing noise, the corresponding error threshold increases from $0.55\%$ to $0.72\%$. Under the hardware-derived error model, we obtain a threshold of $0.80\%$, corresponding to a threshold cooperativity of $C_{\mathrm{th}}=7.8 \times 10^4$, compatible with experimentally accessible parameters for Rydberg-coupled microwave-cavity systems. By avoiding atom transport, the Cat Bus provides a route towards high-speed, fault-tolerant neutral-atom quantum computation.

AI Summary

The paper asks whether cavity-mediated interactions can remove atom-shuttling latency from neutral-atom fault-tolerant computing. It proposes a static atom array coupled to crossed rows and columns of microwave resonators, each stabilized in a bosonic cat manifold. Projecting the resonant atom–cavity interaction into this manifold yields approximately commuting conditional rotations, enabling a native cat–atom $\mathrm{CZ}^n$ gate whose duration is independent of target count at fixed cat amplitude. The analysis derives leading photon-loss and Rydberg-decay channels, with optimized process infidelity $\epsilon_{n,\min}=\pi\sqrt{n/(2C)}$ for cooperativity $C=g^2/(\kappa_1\gamma)$. Assumed parameters give a 142 ns native gate. For hypergraph-product codes, syndrome extraction is compiled through star-based scheduling, with minimum depth within the specified scheduling model determined by a minimum vertex cover. The estimated cycle time scales as $N^{1/2}$ and is 180 times shorter than an atom-rearrangement estimate at $N=10^5$ data qubits. Stabilizer-circuit simulations with BP+OSD decoding give thresholds of approximately $0.72\%$ with cat flags versus $0.55\%$ for rearrangement under matched pairwise depolarizing noise. A hardware-derived stochastic model gives $0.80\%$, mapped to $C_{\mathrm{th}}\approx7.8\times10^4$. These are architectural estimates and quantum-memory simulations, not experimental results. Threshold benchmarks assume ideal single-qubit gates, preparation, measurement and idling, and replace atomic leakage by unheralded depolarizing noise. The channel derivation omits finite-dissipative-gap corrections. Large-code logical failure rates are extrapolated from empirical fits; universal fault-tolerant logical gates remain future work.

Little sign of AI-generated textStrong assumptionsOverclaims

Central claim may not hold: The reported thresholds assume ideal single-qubit gates, preparation, measurement, and idling, so they establish a CZ-limited benchmark rather than a full hardware fault-tolerance threshold. The 0.80% threshold uses independent atomic depolarizing noise in place of the derived leakage channel, leaving its identification with a physical cooperativity threshold unvalidated. The error model omits Rydberg decay during the preparation and return pulses, whose integrated excited-state population adds approximately 35% to the interaction-only decay exposure for the quoted parameters. The 180-fold cycle-time comparison omits atomic check-ancilla preparation and measurement durations without establishing that they are negligible or overlapped. The quoted physical performance relies on strong cat stabilization without a numerical stabilization rate or a bound on the omitted finite-gap errors.

Written by gpt-6.1-sol from the paper's full text. Automated: it can be wrong.

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13+14 pages, 4+6 figures

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The paper asks whether cavity-mediated interactions can remove atom-shuttling latency from neutral-atom fault-tolerant computing. It proposes a static atom array coupled to crossed rows and columns of microwave resonators, each stabilized in a bosonic cat manifold. Projecting the resonant atom–cavity interaction into this manifold yields approximately commuting conditional rotations, enabling a native cat–atom CZn\mathrm{CZ}^nCZn gate whose duration is independent of target count at fixed cat amplitude.
The analysis derives leading photon-loss and Rydberg-decay channels, with optimized process infidelity ϵn,min⁡=πn/(2C)\epsilon_{n,\min}=\pi\sqrt{n/(2C)}ϵn,min​=πn/(2C)​ for cooperativity C=g2/(κ1γ)C=g^2/(\kappa_1\gamma)C=g2/(κ1​γ). Assumed parameters give a 142 ns native gate. For hypergraph-product codes, syndrome extraction is compiled through star-based scheduling, with minimum depth within the specified scheduling model determined by a minimum vertex cover. The estimated cycle time scales as N1/2N^{1/2}N1/2 and is 180 times shorter than an atom-rearrangement estimate at N=105N=10^5N=105 data qubits. Stabilizer-circuit simulations with BP+OSD decoding give thresholds of approximately 0.72%0.72\%0.72% with cat flags versus 0.55%0.55\%0.55% for rearrangement under matched pairwise depolarizing noise. A hardware-derived stochastic model gives 0.80%0.80\%0.80%, mapped to Cth≈7.8×104C_{\mathrm{th}}\approx7.8\times10^4Cth​≈7.8×104.
These are architectural estimates and quantum-memory simulations, not experimental results. Threshold benchmarks assume ideal single-qubit gates, preparation, measurement and idling, and replace atomic leakage by unheralded depolarizing noise. The channel derivation omits finite-dissipative-gap corrections. Large-code logical failure rates are extrapolated from empirical fits; universal fault-tolerant logical gates remain future work.
Efficient quantum error correction and fault-tolerant quantum computing require scalable, high-fidelity long-range connectivity. In neutral-atom quantum computers, this is commonly achieved through atom transport, but shuttling introduces latency and motional heating that worsen with system size. Here, we introduce a neutral-atom architecture based on static atomic buses, in which auxiliary mediator atoms enable long-range entangling operations without qubit transport. The architecture naturally supports long-range stabilizer measurements in high-rate LDPC codes and transversal logical gates between neighboring surface-code patches, enabling a modular framework for efficient logical memories, Clifford computation, and magic-state distillation. To realize these capabilities, we co-design optimal-control protocols for bus-mediated controlled-Z gates that incorporate both microscopic neutral-atom dynamics and architectural constraints. We obtain smooth bus-mediated gates with fidelities approaching 99.9% and durations of a few hundred nanoseconds by combining time-optimal control with interaction-flatness and robustness constraints. Large-scale simulations of quantum error correction and logical entangling operations between neighboring surface-code patches predict more than an order-of-magnitude improvement in logical error rates compared with atom-shuttling architectures under realistic noise. The architecture achieves logical gate times of approximately 100 us and quantum-error-correction cycle times of about 1 ms for code distances d<12. These results establish static atomic buses as a practical alternative to atom shuttling for scalable fault-tolerant neutral-atom quantum computing.
Neutral atom quantum computing utilizes laser-trapped neutral atoms as qubits and realizes quantum logic gate operations through Rydberg-state interactions. In recent years, it has become one of the most vibrant directions in quantum computing hardware. This paper systematically reviews the working principles of neutral-atom quantum computers, including qubit encoding, atom trapping and manipulation, Rydberg states and interactions, the Rydberg blockade quantum gate mechanism, and atom rearrangement with reconfigurable architectures. The mainstream technical routes are surveyed, represented by optical tweezer arrays combined with Rydberg interactions, optical lattice schemes, and dipole trap arrays. A panoramic review is provided of domestic and international research progress from theoretical foundations in 2000 to the latest achievements in 2026, including thousand-qubit-scale systems, logical qubits, and quantum error correction experiments. Key breakthroughs are highlighted, such as the 6100-atom qubit array, continuous operation of a 3000-qubit system, quantum simulation of the Kitaev honeycomb model, toric code error correction demonstrations, encoding rates exceeding 1/2, and fault-tolerant architectures. The core bottlenecks are analyzed in depth, including the scalability--fidelity trade-off, engineering implementation of quantum error correction, atom loss and mid-circuit replenishment, laser system industrialization, control electronics scalability, and long-distance quantum interconnection. This paper aims to provide a systematic reference for academic research and technological development in this field.
We construct a fault-tolerant quantum error-correcting protocol based on a qubit encoded in a large spin qudit using a spin-cat code, analogous to the continuous-variable cat encoding. With this, we can correct the dominant error sources, namely processes that can be expressed as error operators that are linear or quadratic in the components of angular momentum. Such codes tailored to dominant error sources can exhibit superior thresholds and lower resource overheads when compared to those designed for unstructured noise models. A key component is the gate that preserves the rank of spherical tensor operators. Categorizing the dominant errors as phase and amplitude errors, we demonstrate how phase errors, analogous to phase-flip errors for qubits, can be effectively corrected. Furthermore, we propose a measurement-free error-correction scheme to address amplitude errors without relying on syndrome measurements. Through an in-depth analysis of logical gate errors, we establish that the fault-tolerant threshold for error correction in the spin-cat encoding surpasses that of standard qubit-based encodings. We consider a specific implementation based on neutral-atom quantum computing, with qudits encoded in the nuclear spin of 87 Sr , and show how to generate the universal gate set, including the rank-preserving gate, using quantum control and the Rydberg blockade. These findings pave the way for encoding a qubit in a large spin with the potential to achieve fault tolerance, high threshold, and reduced resource overhead in quantum information processing. Published by the American Physical Society 2024
Fault-tolerant quantum computing requires architectures that simultaneously address scalability, connectivity, and error correction under realistic noise constraints. We present a compound photonic-atomic quantum computing platform that uses cavity QED to realize near-deterministic entangling operations between flying photonic qubits and stationary atomic qubits. Photons provide long-range connectivity and scalability via measurement-based quantum computing (MBQC), while atoms supply reusable, near-deterministic resources for photon generation and entanglement, overcoming the inefficiency of purely photonic platforms. The core primitive is a symmetrized Duan-Kimble photon-atom controlled-phase (CZ) gate, robust to experimental imperfections and high-fidelity. Using single 87^{87}87Rb atoms coupled to optical cavities, we give protocols for state preparation, measurement, photon generation, and entangling gates on tens-of-nanosecond timescales, and show how large-scale cluster states with effectively unrestricted connectivity and reduced overhead can be generated through atomic reuse. We analyze fault tolerance on the Raussendorf-Harrington-Goyal (RHG) lattice with a hardware-aware noise model capturing asymmetric loss and correlated photonic-atomic errors. Logical memory simulations yield a photon-loss threshold near 2.6%2.6\%2.6% per physical gate ($\sim$15\% total per trajectory). The full Clifford set -- Hadamard, phase, CNOT -- is implementable transversally or fold-transversally at thresholds matching the identity channel, and we propose two non-Clifford resource-state routes (code teleportation and magic state cultivation) within the foliated cluster-state architecture.
Neutral-atom arrays are a leading qubit technology for large-scale, fault-tolerant quantum computing (FTQC). A dominant error source on this platform is qubit loss, which accrues with every operation and movement. The presence of loss undermines the promises of existing architectural work. Standard error correction targets stochastic Pauli errors and cannot correct loss, so most FTQC performance analyses are not directly compatible with it. Moreover, compilation and routing decisions, which strongly affect overall loss, are typically optimized against Pauli-error cost models and often remain loss-agnostic, potentially increasing exposure to the loss channel. In this work, we comprehensively model the effect of qubit loss on neutral-atom FTQC and develop a loss-tolerant transversal-gate architecture. We treat loss not as a predetermined error parameter but as a dynamic budget spent across a whole program, allowing us to control it by co-designing layout, compilation, and decoding. We target a physical implementation with no separate storage and entangling zones, eliminating the repeated SLM-AOD handoffs and long-distance shuttling that dominate loss in other layouts. We develop compiler optimizations that maximize gate parallelism while respecting the RF tone budget and AOD bandwidth constraints. Our work couples these with a loss-aware, delayed-erasure decoder and an end-to-end loss-aware magic state cultivation protocol. Overall, we improve accumulated loss per syndrome-extraction round by up to 2.15X against a zoned baseline and reduce logical error rates by over two orders of magnitude versus current architectures. Our framework also informs concrete device targets such as continuous reloading rates, AOD counts, and shuttling trajectory choices. We expect these insights to matter for system architects as neutral-atom hardware scales.
Logical qubits can be protected from decoherence by performing QEC cycles repeatedly. Algorithms for fault-tolerant QEC must be compiled to the specific hardware platform under consideration in order to practically realize a quantum memory that operates for in principle arbitrary long times. All circuit components must be assumed as noisy unless specific assumptions about the form of the noise are made. Modern QEC schemes are challenging to implement experimentally in physical architectures where in-sequence measurements and feed-forward of classical information cannot be reliably executed fast enough or even at all. Here we provide a novel scheme to perform QEC cycles without the need of measuring qubits that is fully fault-tolerant with respect to all components used in the circuit. Our scheme can be used for any low-distance CSS code since its only requirement towards the underlying code is a transversal CNOT gate. Similarly to Steane-type EC, we coherently copy errors to a logical auxiliary qubit but then apply a coherent feedback operation from the auxiliary system to the logical data qubit. The logical auxiliary qubit is prepared fault-tolerantly without measurements, too. We benchmark logical failure rates of the scheme in comparison to a flag-qubit based EC cycle. We map out a parameter region where our scheme is feasible and estimate physical error rates necessary to achieve the break-even point of beneficial QEC with our scheme. We outline how our scheme could be implemented in ion traps and with neutral atoms in a tweezer array. For recently demonstrated capabilities of atom shuttling and native multi-atom Rydberg gates, we achieve moderate circuit depths and beneficial performance of our scheme while not breaking fault tolerance. These results thereby enable practical fault-tolerant QEC in hardware architectures that do not support mid-circuit measurements.