<?xml version="1.0" encoding="utf-8"?><feed xmlns="http://www.w3.org/2005/Atom">
  <title>QOC — Control for quantum error correction</title>
  <subtitle>Quantum control papers on arXiv, selected and classified automatically by QOC.</subtitle>
  <id>https://llorebaga.github.io/QOC/topics/error-correction/</id>
<link rel="alternate" type="text/html" href="https://llorebaga.github.io/QOC/topics/error-correction/"/>
  <link rel="self" type="application/atom+xml" href="https://llorebaga.github.io/QOC/topics/error-correction/feed.xml"/>  <updated>2026-10-15T00:00:00Z</updated>
  <generator>QOC</generator>
  <entry>
    <title>Programmable all-to-all entangling gates for cavity-coupled atoms</title>
    <id>https://arxiv.org/abs/2610.22220</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2610.22220"/>
    <published>2026-10-15T00:00:00Z</published>
    <updated>2026-10-15T00:00:00Z</updated>
<author><name>Angus Crookes</name></author><author><name>Ben Yuen</name></author><author><name>Angela Demetriadou</name></author><category term="neutral-atoms" label="Neutral atoms &amp; Rydberg arrays"/><category term="gate-synthesis" label="Quantum gate synthesis"/><category term="photonics" label="Photonic &amp; optomechanical systems"/><category term="error-correction" label="Control for quantum error correction"/>    <summary type="text">Fault tolerant quantum computers greatly benefit from having both high fidelity entangling gates and a non-local qubit connectivity. However, most entangling gates for neutral atoms are local, requiring separated atoms to be moved using optical tweezers to yield entanglement between them. Here, we design a high fidelity Mølmer Sørensen-like entangling gate between neutral atoms coupled to a photonic cavity, enabling a programmable all-to-all connectivity through the shared cavity coupling. The gate is both robust to changes in cavity photon number, and enables selective entanglement between any subset of separated atoms through local laser addressing. This eliminates the need to physically move atoms to perform the gate, and therefore motional errors and erasure are suppressed. Using experimentally realistic parameters we demonstrate gate fidelities exceeding $F &gt; 0.99$, with higher fidelities achievable through optimal control of the pump amplitudes.</summary>
  </entry>
  <entry>
    <title>Dynamical Decoupling of Nonclassical States in a Biased-Noise Spin Qudit</title>
    <id>https://arxiv.org/abs/2610.19676</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2610.19676"/>
    <published>2026-10-14T00:00:00Z</published>
    <updated>2026-10-14T00:00:00Z</updated>
<author><name>Arjen Vaartjes</name></author><author><name>Namit Anand</name></author><author><name>Rocky Y. Su</name></author><author><name>Akram Youssry</name></author><author><name>Ritik Sareen</name></author><author><name>Jeffrey Marshall</name></author><author><name>Mark R. van Blankenstein</name></author><author><name>Danielle Holmes</name></author><author><name>Benjamin Wilhelm</name></author><author><name>Bibek Pokharel</name></author><author><name>Xi Yu</name></author><author><name>Laura A. O&#39;Neill</name></author><author><name>Martin Nurizzo</name></author><author><name>Alexander M. Jakob</name></author><author><name>Fay E. Hudson</name></author><author><name>Kohei M. Itoh</name></author><author><name>Andrew S. Dzurak</name></author><author><name>David N. Jamieson</name></author><author><name>Andrea Morello</name></author><category term="dynamical-decoupling" label="Dynamical decoupling"/><category term="spins" label="Spins — NMR, ESR &amp; colour centres"/><category term="error-correction" label="Control for quantum error correction"/><category term="gate-synthesis" label="Quantum gate synthesis"/>    <summary type="text">Encoding quantum information in $d$-dimensional systems (qudits) with $d&gt;2$ offers appealing new directions for resource-efficient quantum computing. However, protecting the coherence of nonclassical qudit resource states remains an open challenge. Dynamical decoupling (DD) is a well-established technique for extending coherence, but its application to qudits is hindered by the quadratic scaling of the decoupling sequence overhead with the dimension $d$. As a result, demonstrations of qudit DD have so far been limited to low-dimensional qudits. Here, we show that noise-biased qudits enable a nontrivial reduction of this overhead, for example, from quadratic to linear. We perform qudit DD on a model $d=8$ qudit, the nuclear spin of an antimony donor in silicon. We benchmark DD performance on highly nonclassical states such as uniform superpositions, cat states, and Haar random states and measure coherence improvements up to a factor $5$ to $10$. For a spin-cat error correction code, continuous DD extends the coherence time of the logical superposition $|+\rangle_L$ to $225$~ms, compared to $19$~ms under free evolution and $85$~ms with a Hahn echo. This improvement shows that DD sequences tailored to a system&#39;s noise bias can significantly enhance the lifetime of encoded logical qubits.</summary>
  </entry>
  <entry>
    <title>Architecting Instruction Execution for Scalable Fault-Tolerant Quantum Computing</title>
    <id>https://arxiv.org/abs/2610.17058</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2610.17058"/>
    <published>2026-10-12T00:00:00Z</published>
    <updated>2026-10-12T00:00:00Z</updated>
<author><name>Dmitry Filippov</name></author><author><name>Justin Hogaboam</name></author><author><name>Mathias Soeken</name></author><author><name>Raghu Gatta</name></author><author><name>Prakash Murali</name></author><author><name>Matthias Troyer</name></author><category term="control-hardware" label="Control electronics &amp; software stacks"/><category term="pulse-level-compilation" label="Pulse-level compilation"/><category term="superconducting" label="Superconducting circuits"/><category term="error-correction" label="Control for quantum error correction"/>    <summary type="text">Scaling fault-tolerant quantum computing (FTQC) requires orchestrating millions of operations continuously across a tightly coupled classical-quantum control stack. A critical challenge in this orchestration is determining the optimal hardware-software boundary, i.e., the Quantum Instruction Set Architecture (QISA). We focus on cryogenic, fixed-connectivity qubit platforms, such as superconducting and topological Majorana qubits. For these, existing QISA choices either operate at too low a level, violating cryogenic thermal budgets at scale, or at too high a level, imposing unrealizable complexity on the control engine. To reason about these tradeoffs, we introduce the ARIES instruction set hierarchy, which categorizes QISAs into distinct abstraction levels. To systematically evaluate these levels, we develop an end-to-end evaluation toolflow featuring a cycle-accurate classical driver and hardware engine simulator. Using eight quantum applications across superconducting and topological qubit platforms, we measure instruction bandwidth, transceiver power dissipation, and measurement processing overheads. We demonstrate that while physical-level abstractions exceed the thermal limits of dilution refrigerators by orders of magnitude, canonical-level abstractions significantly underestimate hardware routing congestion and execution runtimes. Our Level 4 QISA (local logical operations) offers an optimal architectural balance. As quantum hardware platforms scale toward FTQC in the coming years, our findings provide concrete architectural guidance for the design of their classical control stacks and instruction interfaces.</summary>
  </entry>
  <entry>
    <title>Scalable Exact Non-Pauli Noise Simulation for Fault-Tolerant Quantum Circuits</title>
    <id>https://arxiv.org/abs/2610.15975</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2610.15975"/>
    <published>2026-10-11T00:00:00Z</published>
    <updated>2026-10-11T00:00:00Z</updated>
<author><name>Yuewen Hou</name></author><author><name>Gokul Subramanian Ravi</name></author><category term="error-correction" label="Control for quantum error correction"/><category term="pulse-level-compilation" label="Pulse-level compilation"/>    <summary type="text">Fault-tolerant quantum design relies on simulating noisy quantum error correction (QEC) circuits with hundreds to thousands of physical qubits and large circuit depths. High-throughput stabilizer simulators, such as Stim, are the de facto tools for this regime. However, these simulators typically support only Clifford gates and stochastic Pauli noise. As a result, more realistic device noise models-such as coherent control errors and thermal relaxation-are often approximated using Pauli Twirling. This replacement offers speed but can introduce inaccuracies. To address this, we propose QuasiStim for scalable exact QEC simulation of realistic noise, with QuasiFold as a compiler frontend and DeltaFrame as a sampling backend. QuasiFold lowers sampling overhead by merging equivalent non-Pauli sites in the quantum circuit. DeltaFrame samples the resulting stabilizer trajectories by reusing precomputed predicted references instead of resimulating the full tableau for each shot. QuasiFold can reduce the number of shots by over $100\times$ on bivariate-bicycle (BB) codes. Compared to a per-shot tableau simulator, DeltaFrame is $166\times$--$1331\times$ faster on rotated surface-code memory under coherent $R_Z$ noise as $d$ grows from 5 to 35. QuasiStim also makes the PTA bias measurable: the gap is non-negligible and varies with noise strength, decoder, and circuit schedule. QuasiStim will be open-sourced upon publication at https://github.com/isaachyw/QuasiStim</summary>
  </entry>
  <entry>
    <title>Entanglement detection in dynamical quantum systems</title>
    <id>https://arxiv.org/abs/2610.15021</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2610.15021"/>
    <published>2026-10-10T00:00:00Z</published>
    <updated>2026-10-10T00:00:00Z</updated>
<author><name>Xingjian Zhang</name></author><author><name>Jiayi Wu</name></author><author><name>Jue Xu</name></author><author><name>Qi Zhao</name></author><category term="many-body-control" label="Many-body optimal control"/><category term="error-correction" label="Control for quantum error correction"/><category term="quantum-speed-limits" label="Quantum speed limits"/>    <summary type="text">Quantum science and engineering increasingly target the exploitation and control of large-scale dynamical systems. As system size grows, novel phenomena and quantum advantages emerge, but the resulting many-body dynamics become correspondingly harder to monitor and characterize. In particular, the underlying Hamiltonian often lacks symmetries, and the induced many-body dynamics quickly become hard to track. Focusing on one of the most important quantum features---entanglement---we demonstrate that, for a broad class of common Hamiltonian models, one can design effective witnesses that detect both the presence and structure of entanglement over relatively long evolution times. Inspired by stabilizer-based simulation, we track the evolution of generalized stabilizers of the underlying state and use them to construct linear entanglement witnesses. Through numerical experiments on Heisenberg-type Hamiltonians with up to twelve qubits, we show that the required number of measurement settings can be kept at a modest scale as the system size increases, and entanglement detection remains effective over evolution times that significantly exceed those accessible to naive approaches. The corresponding calculations can be carried out largely symbolically. Furthermore, unlike accurate state simulation, the stabilizer-based design of entanglement witnesses can be performed in a much more coarse-grained, digitized manner. We hope these results will stimulate further exploration of the quantum control of large systems.</summary>
  </entry>
  <entry>
    <title>Protecting bosonic codes from ancilla-induced errors with continuous-variable flags</title>
    <id>https://arxiv.org/abs/2610.07139</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2610.07139"/>
    <published>2026-10-05T00:00:00Z</published>
    <updated>2026-10-05T00:00:00Z</updated>
<author><name>Thomas Décultot</name></author><author><name>Ronan Gautier</name></author><author><name>Mazyar Mirrahimi</name></author><category term="bosonic-control" label="Bosonic &amp; continuous-variable control"/><category term="error-correction" label="Control for quantum error correction"/><category term="superconducting" label="Superconducting circuits"/><category term="trapped-ions" label="Trapped ions"/>    <summary type="text">Bosonic quantum error correction represents a route towards significant hardware overhead reduction for fault-tolerant quantum computation. However, controlling quantum harmonic oscillators that encode the quantum information comes with its own challenges. In many platforms such as superconducting circuits and trapped ions, the bosonic degree of freedom is controlled by an ancillary qubit whose decay during a qubit-oscillator gate propagates to the oscillator as a continuous error. Such errors generally lie beyond the scope of errors that the bosonic code is capable of correcting. We introduce the continuous-variable flag: an auxiliary oscillator coupled to the ancilla whose phase-space position encodes the continuous error corrupting the storage mode. After the gate, a heterodyne measurement of the flag estimates this continuous-variable error and a subsequent feedback control undoes it up to a bosonic code stabilizer. The scheme requires no new ingredients, as the flag is driven by the same dispersive coupling, displacements and rotations that implement the gates it is supposed to protect. We construct sequences protecting conditional rotations to all orders in ancilla decay with one flag, and conditional displacements to first order with one flag and to all orders with two. Simulations with realistic circuit-QED parameters predict more than three orders of magnitude fewer logical errors for the parity measurement of a four-component cat code, and a finite-energy GKP logical lifetime near its noiseless-ancilla bound. By discretizing continuous-variable errors, the flags introduced in this work are a useful tool for any hybrid oscillator-qubit processor, and open the route towards fault-tolerant simulation and computation with bosonic modes.</summary>
  </entry>
  <entry>
    <title>Measurement-free Preparation of Surface-Code States with Digital-Analog Counterdiabatic Drivings</title>
    <id>https://arxiv.org/abs/2610.06697</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2610.06697"/>
    <published>2026-10-05T00:00:00Z</published>
    <updated>2026-10-06T00:00:00Z</updated>
<author><name>Shubham Kumar</name></author><author><name>Balaganchi A. Bhargava</name></author><author><name>Paolo Andrea Erdman</name></author><author><name>Anne-Maria Visuri</name></author><author><name>José D. Martín-Guerrero</name></author><author><name>Yolanda Vives-Gilabert</name></author><author><name>Enrique Solano</name></author><author><name>Narendra N. Hegade</name></author><category term="error-correction" label="Control for quantum error correction"/><category term="state-preparation" label="State preparation &amp; transfer"/><category term="shortcuts-to-adiabaticity" label="Shortcuts to adiabaticity"/><category term="variational-algorithms" label="Variational algorithms &amp; QAOA as control"/>    <summary type="text">Preparing stabilizer-code states with shallow circuits is an important primitive for near-term quantum error correction in superconducting circuits, where logical-state initialization requires four-body stabilizer correlations from native one- and two-body controls. We introduce a digital-analog method for the preparation of surface-code ground-state manifolds. The method exploits a structural property of the adiabatic gauge potential, mapping stabilizer-local counterdiabatic terms to digital-analog blocks on the superconducting layout using fixed-angle two-qubit XY gates, single-qubit rotations, and analog exchange-interaction evolutions. The dressed blocks generate higher-order operators used as the variational ansatz to determine the counterdiabatic terms within the Sels-Polkovnikov adiabatic-gauge-potential framework. We benchmark checkerboard plaquette-stabilizer grids up to 4 x 4; the square-grid instances correspond to rotated surface codes, while the rectangular cases probe the scaling of the method. For all grids, the proposed method generates the dominant four-body counterdiabatic basis and, at short evolution times, substantially improves ground-state preparation compared with bare adiabatic evolution. We further generalize the construction to n x m stabilizer lattices and show that digital-analog synthesis can reduce the entangling depth by an order of magnitude. Together, these results establish a direct connection between stabilizer geometry, the structure of the counterdiabatic gauge potential, and digital-analog control for measurement-free preparation of stabilizer-code states on near-term superconducting architectures.</summary>
  </entry>
  <entry>
    <title>Optimal local recovery cannot alter critical orthogonality exponents in quantum spin environments</title>
    <id>https://arxiv.org/abs/2609.39528</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2609.39528"/>
    <published>2026-09-30T00:00:00Z</published>
    <updated>2026-09-30T00:00:00Z</updated>
<author><name>Zhixuan Zhao</name></author><author><name>Jun Li</name></author><category term="error-correction" label="Control for quantum error correction"/>    <summary type="text">We prove a local amplitude-ratio bound for positive ground states and an explicit reverse comparison for fidelity under finite-region erasure. An exact lattice calculation for a connected critical Ising chain gives amplitude exponent $1/8$, preserved by arbitrary optimal control on any fixed spin set and, at the level of logarithmic exponents, on $o(\log N)$ spins. We derive the finite Cauchy product and its uniform strip asymptotics, and document exact two-spin optimization and an interferometric protocol for measuring the recovery. A separate finite-mediator theorem quantifies local compression and a decoder while retaining the rest of the environment exactly. We also give a ground-preparation Ramsey bound, counterexamples to stronger projected-state inferences, and independent full-Hamiltonian calculations.</summary>
  </entry>
  <entry>
    <title>Preparation Changes the Cost of Calibration for Quantum Control</title>
    <id>https://arxiv.org/abs/2609.30910</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2609.30910"/>
    <published>2026-09-25T00:00:00Z</published>
    <updated>2026-09-25T00:00:00Z</updated>
<author><name>Xiu-Hao Deng</name></author><category term="error-correction" label="Control for quantum error correction"/><category term="closed-loop" label="Closed-loop &amp; in-situ optimization"/>    <summary type="text">Error-correction records can reveal noise yet supply the information needed for control too slowly. In a surface code under Gaussian dephasing, encoded calibration learns a correlation that reverses the preferred control mainly through rare events. A product probe exposes it more often through the same checks, reducing ideal-record sample complexity from inverse-square to inverse-linear in phase variance. Counting both calibration and execution costs, we show that this gain can repay probe overhead and enable protected tasks within budgets that exclude encoded calibration.</summary>
  </entry>
  <entry>
    <title>Pulse-Level Compilation of Measurement-Free Recovery in Transmon Circuits</title>
    <id>https://arxiv.org/abs/2609.16133</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2609.16133"/>
    <published>2026-09-14T00:00:00Z</published>
    <updated>2026-09-14T00:00:00Z</updated>
<author><name>Yi-Han Yu</name></author><author><name>Kai Xu</name></author><author><name>Heng Fan</name></author><category term="pulse-level-compilation" label="Pulse-level compilation"/><category term="error-correction" label="Control for quantum error correction"/><category term="superconducting" label="Superconducting circuits"/>    <summary type="text">Quantum error correction commonly relies on syndrome measurement, decoding, and conditional feedback. We numerically show that the conditional spectrum of an interacting transmon circuit can compile a local recovery rule into a fixed open-loop control cycle. In a four-bit repetition-code ring, the resulting input-independent control slows the decay of logical coherence under Pauli-\(X\) noise and stabilizes logical-one population under data relaxation relative to uncorrected references. Its local, bounded-degree architecture provides a hardware-native framework for extending compiled recovery control to larger quantum networks.</summary>
  </entry>
  <entry>
    <title>Engineering dissipation and control pulses for high-fidelity fault-tolerance quantum computing</title>
    <id>https://arxiv.org/abs/2609.15477</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2609.15477"/>
    <published>2026-09-14T00:00:00Z</published>
    <updated>2026-09-14T00:00:00Z</updated>
<author><name>Shao-Wei Xu</name></author><author><name>Zhe-Yuan Zhang</name></author><author><name>Yi-Tong Shi</name></author><author><name>Ye-Hong Chen</name></author><author><name>Yan Xia</name></author><category term="bosonic-control" label="Bosonic &amp; continuous-variable control"/><category term="error-correction" label="Control for quantum error correction"/><category term="shortcuts-to-adiabaticity" label="Shortcuts to adiabaticity"/><category term="robust-optimal-control" label="Robust &amp; ensemble optimal control"/>    <summary type="text">Cat-state qubits, a prominent class of bosonic encodings, offer a promising pathway toward hardware-efficient fault-tolerant quantum computing. In this manuscript, we propose an optimally robust control protocol for the cat-state qubits which are stabilized by engineering two-photon dissipation. By deriving an effective two-level description in the cat-state subspace and applying shortcut-to-adiabaticity via inverse engineering, we design a robust protocol to achieve fast and high-fidelity state transfer in the cat-state qubit. We analyze the sensitivity to systematic control errors and identify an optimal robustness condition that strongly suppresses errors induced by imperfections in the driving fields. Furthermore, we show that dissipative confinement efficiently suppresses leakage out of the cat-state subspace caused by the pure dephasing, highlighting an intrinsic advantage of dissipative-cat qubits. This work establishes a robust and leakage-suppressing framework for high-fidelity bosonic qubit control, offering a promising route toward scalable fault-tolerant quantum computing.</summary>
  </entry>
  <entry>
    <title>Detuning-robust Rydberg entangling gates from echoed pulses</title>
    <id>https://arxiv.org/abs/2608.26446</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2608.26446"/>
    <published>2026-08-26T00:00:00Z</published>
    <updated>2026-09-02T00:00:00Z</updated>
<author><name>Zhubing Jia</name></author><author><name>Yichao Yu</name></author><author><name>Xiye Hu</name></author><author><name>Lintao Li</name></author><author><name>Jacob Zheng</name></author><author><name>Christopher Monroe</name></author><author><name>Jacob P. Covey</name></author><category term="neutral-atoms" label="Neutral atoms &amp; Rydberg arrays"/><category term="gate-synthesis" label="Quantum gate synthesis"/><category term="error-correction" label="Control for quantum error correction"/>    <summary type="text">Rydberg-based two-qubit gate fidelities in neutral atom arrays are limited chiefly by laser intensity inhomogeneity and by detuning errors from frequency miscalibration, background-field drift, intermediate state light shift and Doppler shifts. Quantum optimal control can suppress the former, but no pulse can render a controlled-Z gate first-order insensitive to detuning. Here we show that this obstruction can be circumvented by designing Rydberg gate pulses with every leading-order detuning error relegated to single-qubit Z-rotations, which an echoed sequence removes. The resulting maximally-entangling ZZ gate has no leading-order response to arbitrary detunings on either atom, maintaining an infidelity below $10^{-3}$ within a much wider range of single-atom detunings than the time-optimal gates. We further show that a large fraction of residual error is dominated by population outside the computational subspace, which can be converted into heralded erasures. Our results significantly reduce the requirements on laser frequency stability and intensity homogeneity, field calibration and atomic temperature toward practical fault-tolerant quantum computing with neutral atoms.</summary>
  </entry>
  <entry>
    <title>High-Fidelity Entangled States in a Connectivity-Four Fluxonium Quantum Processor</title>
    <id>https://arxiv.org/abs/2608.25503</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2608.25503"/>
    <published>2026-08-26T00:00:00Z</published>
    <updated>2026-08-26T00:00:00Z</updated>
<author><name>Johannes Schirk</name></author><author><name>Niklas Bruckmoser</name></author><author><name>S. M. Taubenberger</name></author><author><name>Florian Wallner</name></author><author><name>Niklas J. Glaser</name></author><author><name>M. Zetzl</name></author><author><name>L. Huang</name></author><author><name>Ivan Tsitsilin</name></author><author><name>Max Werninghaus</name></author><author><name>Lasse Södergren</name></author><author><name>Klaus Liegener</name></author><author><name>Christian Schneider</name></author><author><name>Stefan Filipp</name></author><category term="gate-synthesis" label="Quantum gate synthesis"/><category term="error-correction" label="Control for quantum error correction"/><category term="state-preparation" label="State preparation &amp; transfer"/><category term="superconducting" label="Superconducting circuits"/>    <summary type="text">A central challenge in fluxonium-based quantum processors is the extension of the qubit connectivity to two-dimensional lattices compatible with quantum code-error correction. Here, we present a fluxonium quantum processor that employs lumped-element resonator couplers which realizes, for the first time, a connectivity-four unit cell with suppressed parasitic interactions. We achieve parallel single-qubit gate fidelities exceeding 99.9 % in simultaneous randomized benchmarking experiments, while maintaining residual static ZZ interactions below 1 kHz across all coupled qubit pairs. We implement resonator-induced phase (RIP) gates and benchmark two-qubit gate fidelities exceeding 99 % using interleaved randomized benchmarking. To cancel spectator errors observed in two-qubit operations, we implement a refocused RIP gate, recovering coherent control in the presence of multi-qubit connectivity. Furthermore, we prepare Greenberger-Horne-Zeilinger states of up to five qubits with a tomographic fidelity of 90 %, verifying multi-qubit entanglement within the unit cell. These results establish the fluxonium-resonator-fluxonium architecture as a viable approach to realizing densely connected fluxonium processors and provide a scalable path toward quantum error-correction-compatible processor architectures.</summary>
  </entry>
  <entry>
    <title>Optimized EIT-Based Multi-Target CNOT^k Gates in Heteronuclear Rydberg Atom Arrays</title>
    <id>https://arxiv.org/abs/2608.15033</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2608.15033"/>
    <published>2026-08-15T00:00:00Z</published>
    <updated>2026-08-15T00:00:00Z</updated>
<author><name>Zeyu Zhou</name></author><author><name>Xian-Lei Sheng</name></author><author><name>Peng Xu</name></author><author><name>Jian Cui</name></author><category term="neutral-atoms" label="Neutral atoms &amp; Rydberg arrays"/><category term="error-correction" label="Control for quantum error correction"/><category term="gate-synthesis" label="Quantum gate synthesis"/><category term="photonics" label="Photonic &amp; optomechanical systems"/>    <summary type="text">Efficient stabilizer readout requiring multi-qubit coupling is a core bottleneck for quantum error correction. One feasible method is direct implementation of the controlled-U gate between one ancilla qubit and the data qubits assigned to stabilizer U measurements. We systematically analyze the native multi-target $\mathrm{C}^1\mathrm{NOT}^k$ gates proposed by Müller et al., which is realized via electromagnetically induced transparency (EIT) and Rydberg blockade mechanisms. Using a microscopic open-system model, we analyze the gate&#39;s scaling with target number k and identify spontaneous emission, Doppler dephasing, target atom inter-coupling, and technical noise as major error contributions. We further optimize the protocol combining two-photon STIRAP control, heteronuclear interaction engineering, and waveform optimization. Our optimized heteronuclear protocol reaches fidelities of 98.03% ($\mathrm{C}^1\mathrm{NOT}^{1}$) and 96.54% ($\mathrm{C}^1\mathrm{NOT}^{4}$), in the presence of all primary noise sources and realistic experimental parameters. These results demonstrate that EIT-based multi-target gates serve as a practical building block for low-depth stabilizer readout.</summary>
  </entry>
  <entry>
    <title>Pulse Engineering of Quantum Many-Body Dynamics: Emergent Scar States, Entanglement, and Nonstabilizerness</title>
    <id>https://arxiv.org/abs/2608.12559</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2608.12559"/>
    <published>2026-08-12T00:00:00Z</published>
    <updated>2026-08-12T00:00:00Z</updated>
<author><name>Prasant Mallik</name></author><author><name>Arkaprava Sil</name></author><author><name>Sudipto Singha Roy</name></author><category term="many-body-control" label="Many-body optimal control"/><category term="error-correction" label="Control for quantum error correction"/><category term="floquet-engineering" label="Floquet engineering &amp; periodic driving"/>    <summary type="text">Understanding and coherently controlling the properties of interacting quantum many-body systems is a central challenge in non-equilibrium quantum physics. While in the past decades, a wide range of many-body Hamiltonians have been introduced to study quantum chaos, atypical eigenstates, and quantum resources, systematically engineering and continuously tuning these properties within a single microscopic model remains largely unexplored. Here, we employ a pulse engineering scheme to construct an effective Hamiltonian that continuously interpolates between a chaotic Heisenberg (XXX) chain with a local impurity and the ZX Hamiltonian. Along this interpolation, we identify several families of analytically tractable atypical eigenstates embedded in the excited-state spectrum with distinct entanglement and nonstabilizerness properties. In the XXX limit, these states exhibit exact plateaus in both entanglement and stabilizer Rényi entropy and correspond to coherent superpositions of long-range valence-bond solid (VBS) states. As the pulse strength increases, the effective Hamiltonians exhibit a hierarchy of new set of approximate entanglement plateaus in the low-energy spectrum. Interestingly, in the fully pulse-engineered ZX limit, we uncover a distinct pair of long-range entangled stabilizer eigenstates, corresponding to rainbow scar states. We further show that pulse engineering preserves the distinct chaotic and non-chaotic regimes of the original model, while that is largely absent in the dynamical generation of entanglement and nonstabilizerness. The pulse-engineered models generate nearly identical quantum resources in both regimes, revealing a partial decoupling between quantum chaos and quantum-resource generation. Our results establish pulse engineering as a versatile framework for generating many-body Hamiltonians with structured eigenstates and tunable quantum resources.</summary>
  </entry>
  <entry>
    <title>QCORE: A Quantum-Control-Oriented Real-Time Execution Architecture with Extensible Closed-Loop Services and Shared AI Acceleration</title>
    <id>https://arxiv.org/abs/2608.06875</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2608.06875"/>
    <published>2026-08-07T00:00:00Z</published>
    <updated>2026-08-07T00:00:00Z</updated>
<author><name>Heyue Li</name></author><author><name>Yanshu Guo</name></author><author><name>Qichun Liu</name></author><author><name>Tie-Fu Li</name></author><author><name>Zhihua Wang</name></author><author><name>Hanjun Jiang</name></author><category term="error-correction" label="Control for quantum error correction"/><category term="closed-loop" label="Closed-loop &amp; in-situ optimization"/><category term="control-hardware" label="Control electronics &amp; software stacks"/><category term="feedback-control" label="Measurement-based feedback"/>    <summary type="text">Scalable quantum processors require control, readout, feedback, calibration, and error correction to coexist under bounded latency and shared-resource constraints, whereas existing platforms typically optimize only a subset of these capabilities. This article presents QCORE (Quantum-Control-Oriented Real-Time Execution), a QPU-side digital control reference architecture positioned between the Host and a platform-specific analog/mixed-signal front end. QCORE separates task management, shared resources, hard-real-time execution, and long-timescale services into four hardware partitions. A fast-result sideband closes same-round feedback, a Measurement Packet provides a traceable measurement and service interface, and a common service-control skeleton, Tile-local QEC, and versioned safe-point commit organize calibration, error correction, and long-term state updates. Transaction-level, event-driven, and quantum-behavioral models are used for evaluation. At a background load of 0.8, the $P_{99}$ latency of the shared Measurement Packet/Event feedback path is $(1.984\pm0.004)L_{\max}$. Closed-loop operation reduces the mean frequency error by $83.2\%\pm0.8\%$ and lowers the state-assignment error at maximum readout drift from $10.39\%\pm0.54\%$ to $5.37\%\pm0.29\%$. No unsafe acceptance or mixed-version observation is observed in 100,000 configuration transactions, and Tile-local QEC reduces modeled global-boundary demand and yields a $2.08\times$ capacity-normalized scaling estimate.</summary>
  </entry>
  <entry>
    <title>Provably Efficient Self-Calibrating Quantum Fault Tolerance</title>
    <id>https://arxiv.org/abs/2608.05686</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2608.05686"/>
    <published>2026-08-06T00:00:00Z</published>
    <updated>2026-08-20T00:00:00Z</updated>
<author><name>Weiyuan Gong</name></author><author><name>Hong-Ye Hu</name></author><category term="error-correction" label="Control for quantum error correction"/><category term="neutral-atoms" label="Neutral atoms &amp; Rydberg arrays"/><category term="closed-loop" label="Closed-loop &amp; in-situ optimization"/><category term="pulse-level-compilation" label="Pulse-level compilation"/>    <summary type="text">Quantum error correction protects logical information only when every physical operation remains below the fault-tolerance threshold, a condition that must be maintained continuously rather than only at the initial calibration. In practice, however, analog control parameters inevitably drift because of environmental fluctuations. As future fault-tolerant quantum computations are expected to run for days or even months, interrupting computation for repeated recalibration becomes fundamentally impractical. A promising alternative is to integrate calibration directly into computation by repurposing syndrome measurements as a calibration signal (Sivak et al, Nature 2026), but whether such self-calibration can be achieved with provable efficiency remains an open question. Here we establish a theoretical framework for such self-calibrating quantum fault tolerance. We prove that, for a broad class of control-induced errors, the detection rate defines a locally strongly convex surrogate objective for analog calibration with high probability. This geometric property enables a simple and efficient online optimization algorithm using only syndrome measurements collected during normal error correction. We prove convergence to an $\varepsilon$ detection rate within $O(1/\varepsilon^2)$ epochs for time-independent drifts and also establish guarantees for time-dependent drifts. We further show that the convergence rate is independent of the code distance for quantum low-density parity-check (LDPC) codes. Pulse-level simulations of neutral-atom arrays and large-scale circuit-level Clifford simulations confirm these theoretical predictions. Our results establish self-calibrating fault tolerance as a provably efficient paradigm in which the same syndrome measurements simultaneously protect logical information and stabilize the underlying hardware.</summary>
  </entry>
  <entry>
    <title>Constructive realization of self-referential prediction limits in quantum control: Resource bounds and Gödel-safe architectures</title>
    <id>https://arxiv.org/abs/2608.04779</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2608.04779"/>
    <published>2026-08-05T00:00:00Z</published>
    <updated>2026-08-05T00:00:00Z</updated>
<author><name>Salman Sajad Wani</name></author><author><name>Álvaro Perales-Eceiza</name></author><author><name>Saif Al-Kuwari</name></author><author><name>Mir Faizal</name></author><category term="error-correction" label="Control for quantum error correction"/><category term="feedback-control" label="Measurement-based feedback"/>    <summary type="text">Programmable quantum control systems increasingly rely on predictive modules for certification, real-time feedback, and autonomous decision-making. This development raises a fundamental question: can self-analyzing quantum platforms universally predict their own experimental outcomes? Wolpert formalized a general impossibility of universal self-prediction. Here we translate that limitation into an explicit laboratory obstruction that can be realized with finite resources. We consider settings with programmable quantum control in which predictors can be embedded as subroutines within the experiments they analyze. Our diagonal construction uses Kleene&#39;s recursion theorem to transform any deterministic bounded-time predictor into a reversible protocol encoding its own specification. The resulting protocol invokes the predictor on that specification and deterministically produces a classical pointer record that contradicts the forecast. For efficient predictors, the compilation has polynomial overhead and admits concrete physical realizations as a fault-tolerant quantum circuit and as a minimal Mach-Zehnder interferometer. These realizations connect computability-theoretic self-reference to programmable quantum hardware. We also introduce and formally define Gödel-safe architectures. These architectures block the forbidden causal path from the protocol description to an actuator that can affect the pointer during the same run. We analyze their implications for real-time quantum error correction, including the resulting expressiveness trade-offs. As quantum control loops grow in computational expressiveness, the limits of self-reference cease to be mere mathematical abstractions and become explicit engineering constraints for the reliable operation of autonomous quantum technologies.</summary>
  </entry>
  <entry>
    <title>Noise-resilient and Scalable Quantum Error Correction for Nuclear Spin Qubits in Silicon with Electron Shuttling</title>
    <id>https://arxiv.org/abs/2607.27527</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2607.27527"/>
    <published>2026-07-29T00:00:00Z</published>
    <updated>2026-07-29T00:00:00Z</updated>
<author><name>Wayne M. Witzel</name></author><author><name>Matthew D. Grace</name></author><author><name>Dwight R. Luhman</name></author><category term="spins" label="Spins — NMR, ESR &amp; colour centres"/><category term="error-correction" label="Control for quantum error correction"/><category term="quantum-sensing" label="Control for sensing &amp; metrology"/><category term="robust-optimal-control" label="Robust &amp; ensemble optimal control"/>    <summary type="text">Nuclear spin qubits in silicon are well-isolated from their environment. Consequently, they have very long lifetimes and low sensitivity to noise, but this also suggests that control and measurement is challenging. We introduce electron pair interferometry (EPI), a protocol to overcome this challenge and maintain robustness to noise. EPI is implemented using an array of quantum dots with isoelectronic nuclear spin qubits located in the dots. A pair of electrons are initialized into a singlet ground state, split apart, and shuttled to the dots containing nuclear spin qubits. We show it is possible to coherently transfer the parity of the nuclei onto the measurable state of singlet/triplet-encoded electrons. Global nuclear magnetic resonance (NMR) can be used to change bases and implement dynamical decoupling (DD). Combined with selective hyperfine-induced $Z_π$ rotations, our gate set is complete for universal quantum computation, tailored to Calderbank-Shor-Steane (CSS) quantum error correction, and robust to noise. We discuss very low sensitivity to charge noise and study the sensitivity to both DC and AC magnetic field inhomogeneity which depends strongly on their relative strengths.</summary>
  </entry>
  <entry>
    <title>Correlated Coherent Errors in Stabilizer Codes: A General Cumulant Framework and Interference-Based Error Suppression</title>
    <id>https://arxiv.org/abs/2607.22503</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2607.22503"/>
    <published>2026-07-24T00:00:00Z</published>
    <updated>2026-07-24T00:00:00Z</updated>
<author><name>Rohan N Rajmohan</name></author><author><name>Antoine Brillant</name></author><author><name>Peter Groszkowski</name></author><author><name>Alireza Seif</name></author><author><name>Jens Koch</name></author><author><name>Aashish A. Clerk</name></author><category term="error-correction" label="Control for quantum error correction"/><category term="dynamical-decoupling" label="Dynamical decoupling"/>    <summary type="text">Coherent errors in stabilizer codes are often correlated across qubits and QEC cycles. Having a general analytical treatment of such noise would thus be extremely valuable. We derive here the exact logical channel induced by repeated QEC cycles under correlated coherent $Z$ noise, and develop a broadly general cumulant-expansion framework that yields a tractable expression for the noise-averaged logical infidelity. Crucially, this expression is non-perturbative in the noise, and applies to arbitrary stabilizer codes and correlation structures. It reveals a feature with no analogue in standard stochastic Pauli error models: the induced channel depends on which stabilizer eigenspace is chosen as the codespace. Exploiting this, we introduce protected stabilizer eigenspace (PROSE) encoding, an error-suppression strategy that selects the optimal codespace. We show that this eigenspace can be efficiently identified in many relevant situations. Further, when combined with logical Pauli twirling, PROSE matches or outperforms standard error suppression techniques (dynamical decoupling, Pauli twirling of physical qubits). We also show that noise correlations, usually assumed to be harmful to QEC, can instead be a resource: with the right encoding, even positive correlations reduce the logical infidelity below the uncorrelated baseline. Our results offer a new, broadly applicable lens on correlated coherent noise in stabilizer codes.</summary>
  </entry>
  <entry>
    <title>Fault-tolerant quantum computation with static atomic buses</title>
    <id>https://arxiv.org/abs/2607.02804</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2607.02804"/>
    <published>2026-07-02T00:00:00Z</published>
    <updated>2026-09-04T00:00:00Z</updated>
<author><name>Matteo Bergonzoni</name></author><author><name>Laura Pecorari</name></author><author><name>Sam Norrell</name></author><author><name>Cody Poole</name></author><author><name>Guido Pupillo</name></author><author><name>Mark Saffman</name></author><category term="error-correction" label="Control for quantum error correction"/><category term="neutral-atoms" label="Neutral atoms &amp; Rydberg arrays"/><category term="gate-synthesis" label="Quantum gate synthesis"/>    <summary type="text">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&lt;12. These results establish static atomic buses as a practical alternative to atom shuttling for scalable fault-tolerant neutral-atom quantum computing.</summary>
  </entry>
  <entry>
    <title>All about quantum error correction: distillation, mitigation, self-correction and beyond</title>
    <id>https://arxiv.org/abs/2606.14034</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2606.14034"/>
    <published>2026-06-12T00:00:00Z</published>
    <updated>2026-06-12T00:00:00Z</updated>
<author><name>D. -S. Wang</name></author><category term="error-correction" label="Control for quantum error correction"/><category term="dynamical-decoupling" label="Dynamical decoupling"/>    <summary type="text">In this work, it is shown that many quantum error-manipulating techniques, such as distillation, error mitigation, and dynamical decoupling, are special cases of the most general framework for quantum error correction. This unifying perspective is achieved by extending quantum error correction to include state-adaptive and channel-adaptive settings, as well as multi-stage coding scenarios. Based on this insight, a model of self-correcting quantum memory is also proposed. This work clarifies the relationship among these techniques and illustrates, through explicit constructions, how the unified perspective can guide the design of reliable quantum information systems.</summary>
  </entry>
  <entry>
    <title>Achieving Heisenberg limit under noisy conditions with quantum Zeno dynamics and dynamical decoupling</title>
    <id>https://arxiv.org/abs/2606.13205</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2606.13205"/>
    <published>2026-06-11T00:00:00Z</published>
    <updated>2026-08-31T00:00:00Z</updated>
<author><name>Ke Zeng</name></author><author><name>Bakmou Lahcen</name></author><author><name>Yu Jiang</name></author><author><name>Kok Chuan Tan</name></author><category term="quantum-sensing" label="Control for sensing &amp; metrology"/><category term="dynamical-decoupling" label="Dynamical decoupling"/><category term="error-correction" label="Control for quantum error correction"/><category term="feedback-control" label="Measurement-based feedback"/>    <summary type="text">Quantum Zeno dynamics (QZD) and dynamical decoupling (DD) are useful tools that enable the effective suppression of noise in quantum systems. We consider the problem of when (i) noise can be suppressed and (ii) Heisenberg limit (HL) can be achieved in quantum metrology, and prove necessary and sufficient conditions for when QZD and DD are useful for achieving these two goals. We further show this condition can hold even when the Hamiltonian-not-in-Lindblad-span (HNLS) condition fails, allowing QZD/DD to recover Heisenberg scaling beyond what is certified by the usual HNLS-based quantum error correction (QEC) criterion. Finally, we demonstrate that the combination of both techniques can allow individually imperfect QZD and DD strategies to saturate HL.</summary>
  </entry>
  <entry>
    <title>Correlation-Assisted Odd-Parity Encoded Gates in Coupled Fluxonium Qubits under Non-Markovian TLS Noise</title>
    <id>https://arxiv.org/abs/2606.07699</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2606.07699"/>
    <published>2026-06-05T00:00:00Z</published>
    <updated>2026-06-05T00:00:00Z</updated>
<author><name>Chenghong Ji</name></author><author><name>Chaoying Zhao</name></author><category term="error-correction" label="Control for quantum error correction"/><category term="open-system-control" label="Control of open quantum systems"/><category term="pulse-level-compilation" label="Pulse-level compilation"/><category term="superconducting" label="Superconducting circuits"/>    <summary type="text">Correlated longitudinal noise can be partially converted into common-mode fluctuations in an oddparity two-qubit subspace. We analyze an encoded logical qubit formed by the states in two coupled fluxonium qubits. Projecting the exchange-coupled two-qubit Hamiltonian onto this subspace yields an effective logical Hamiltonian in which the exchange interaction drives XL rotations and the qubit detuning drives ZL rotations. We model correlated two-levelsystem (TLS) noise by using longitudinal stochastic processes with finite memory time and evaluate encoded-gate performance through the average gate fidelity. Within the projected model, positive spatial noise correlation suppresses the differential fluctuation and thereby improves the fidelity of encoded logical gates. We further compare Gaussian Ornstein-Uhlenbeck, Markovian, and randomtelegraph noise models and examine the role of logical dynamical decoupling. These results identify a noise-adapted control mechanism for odd-parity encoded operations in coupled fluxonium devices and motivate future multilevel simulations including leakage and pulse-level constraints.</summary>
  </entry>
  <entry>
    <title>Quantum optimization beyond QUBO for industrial logistics and scheduling</title>
    <id>https://arxiv.org/abs/2605.30252</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2605.30252"/>
    <published>2026-05-28T00:00:00Z</published>
    <updated>2026-05-28T00:00:00Z</updated>
<author><name>Juan F. R. Hernández</name></author><author><name>Pavle Nikačević</name></author><author><name>Enrique Solano</name></author><author><name>Chinonso Onah</name></author><author><name>Agneev Guin</name></author><author><name>Arne-Christian Voigt</name></author><author><name>Archismita Dalal</name></author><category term="error-correction" label="Control for quantum error correction"/><category term="pulse-level-compilation" label="Pulse-level compilation"/>    <summary type="text">The increasing complexity of industrial scheduling and transport routing problems motivates the study of alternative optimization formulations and computational paradigms. In this work, we study how higher-order unconstrained binary optimization (HUBO) formulations of such problems map onto quantum optimization workflows in both noisy and fault-tolerant regimes. We consider three representative logistics and manufacturing use cases and formulate each as a HUBO problem. This captures process intricacies, such as highly correlated assembly-line scheduling rules, which are difficult to express faithfully with the standard quadratic (QUBO) form, while at the same time reducing the number of binary variables required in the quantum mapping, thus lowering qubit demand. We compare the HUBO formulations with corresponding QUBO encodings, highlighting a key trade-off: while HUBO reduces qubit requirements through compact binary encoding, it introduces higher-order interaction terms that increase circuit depth, limiting feasibility on current quantum hardware. The proposed formulations are validated using classical solvers across several problem instances and benchmark small routing problem instances using bias-field digitized counterdiabatic quantum optimization in classical simulation. We complement these results with a resource and scalability analysis, focusing on the capacitated vehicle routing problem as a representative large-scale industrial use case. Our analysis indicates that while HUBO formulations offer advantages in qubit scaling compared to QUBO encodings, their practical implementation is constrained by gate fidelity, coherence, and circuit depth, making hybrid quantum-classical workflows and early fault-tolerant quantum hardware the most plausible settings for their practical use.</summary>
  </entry>
  <entry>
    <title>Hardware-Tailored Resource Estimation for Magic-State Distillation on Silicon Spin Qubits</title>
    <id>https://arxiv.org/abs/2605.28936</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2605.28936"/>
    <published>2026-05-27T00:00:00Z</published>
    <updated>2026-05-27T00:00:00Z</updated>
<author><name>Songqinghao Yang</name></author><author><name>Christopher K. Long</name></author><author><name>Rubén M. Otxoa</name></author><author><name>Prakash Murali</name></author><author><name>Crispin H. W. Barnes</name></author><author><name>David R. M. Arvidsson-Shukur</name></author><category term="spins" label="Spins — NMR, ESR &amp; colour centres"/><category term="error-correction" label="Control for quantum error correction"/>    <summary type="text">We present a resource analysis for generating high-fidelity logical magic states on silicon spin-qubit platforms. We consider a range of architectures, including a shuttling-based SpinBus design, a dense nearest-neighbor layout, and a hybrid scheme with shuttling-connected patches. We compare surface, color, and biased error-correcting codes, and analyze the $5\to1$ and $15\to1$ magic-state distillation protocols. Our approach combines bottom-up and top-down methodologies. We construct a hardware-level noise model based on a silicon-processor Hamiltonian with realistic parameters and $1/f$ non-Markovian noise, enabling estimation of physical resources required to reach target logical error rates. These results are propagated to system-level overheads for applications including spin dynamics, integer factorization, and quantum chemistry. Conversely, we fix target logical fidelities and derive corresponding constraints on hardware performance. Our framework enables systematic evaluation of resource-reduction strategies. We find that optimized control pulses reduce magic-state distillation overhead by 42\% compared to standard gate implementations. In addition, silicon-tailored biased error-correcting codes achieve an approximately threefold reduction in physical footprint relative to the surface code, even without physical-bias-preserving operations.</summary>
  </entry>
  <entry>
    <title>Crystallographic Symmetry Generates Phononic Holonomic Gates with Biased-Erasure Channels</title>
    <id>https://arxiv.org/abs/2605.10932</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2605.10932"/>
    <published>2026-05-11T00:00:00Z</published>
    <updated>2026-05-11T00:00:00Z</updated>
<author><name>El Mustapha Mansouri</name></author><author><name>Keigo Arai</name></author><category term="error-correction" label="Control for quantum error correction"/><category term="shortcuts-to-adiabaticity" label="Shortcuts to adiabaticity"/><category term="drag" label="DRAG &amp; leakage suppression"/><category term="dynamical-decoupling" label="Dynamical decoupling"/>    <summary type="text">Solid-state processors require control layers whose errors are legible to quantum-error-correction decoders. We show that crystallographic symmetry can provide such a layer in strain-active Lambda manifolds. When the projected strain tensor and Lambda-transition operators share a multiplicity-one two-dimensional irreducible representation, symmetry fixes the linear strain interaction to a scalar dot product. Two phase-locked mechanical modes synthesize a circular strain field, enabling complex phononic Lambda-leg control without local microwave near fields. On this manifold we construct a superadiabatic echo-lune holonomic gate using Lambda-leg control and a resonant double-quantum counterdiabatic tone. Rotating-frame simulations of a nitrogen-vacancy center give 99.88% conditional average fidelity in 1.833 microseconds, or 99.40% when leakage is counted as error. A resonant gigahertz high-overtone bulk acoustic resonator analysis translates the Hamiltonian into Rabi-rate, linewidth, and envelope-tracking requirements. The bright-state structure organizes noise: A2-sector perturbations are parity-filtered into an optically distinguishable auxiliary state, whereas transverse E-sector faults are echo suppressed and retained as a decoder stress axis. The extracted channel has 0.47% erasure probability and 0.168% residual Z error. In XZZX code-capacity simulations, this biased-erasure model yields a nominal 64% fit-extrapolated data-qubit reduction relative to an unstructured Rabi baseline. Repeated-round detector-model diagnostics preserve the nominal distance-9 proxy and identify missed erasures, transverse floors, leakage/flag timing, and strong crosstalk as validation limits. Extensions to orbital Lambda systems and bright-projector phonon-bus diagnostics identify crystallographic symmetry as a principle for co-designing phononic actuation, leakage, noise bias, and quantum decoding.</summary>
  </entry>
  <entry>
    <title>Multi-Qubit Stabilizer Readout on a Dual-Species Rydberg Array</title>
    <id>https://arxiv.org/abs/2605.10924</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2605.10924"/>
    <published>2026-05-11T00:00:00Z</published>
    <updated>2026-05-11T00:00:00Z</updated>
<author><name>Yu Wang</name></author><author><name>Ryan Cimmino</name></author><author><name>Kenneth Wang</name></author><author><name>Santiago Lopez</name></author><author><name>Jeffrey Li</name></author><author><name>Jin Ming Koh</name></author><author><name>Jonathan N. Hallén</name></author><author><name>Anne Matthies</name></author><author><name>Norman Y. Yao</name></author><author><name>Kang-Kuen Ni</name></author><category term="neutral-atoms" label="Neutral atoms &amp; Rydberg arrays"/><category term="error-correction" label="Control for quantum error correction"/><category term="closed-loop" label="Closed-loop &amp; in-situ optimization"/>    <summary type="text">The ability to locally control and measure subsets of ancilla qubits in an efficient and crosstalk-free manner is a key ingredient in quantum error correction (QEC). Dual-species neutral atom arrays offer an ideal implementation of these capabilities, enabling independent state preparation, manipulation, and detection on each species. In this work, we realize such a dual-species Rydberg array of Na and Cs atoms trapped in co-localized 2D optical tweezer arrays, using Na as an ancilla to measure stabilizers of surrounding Cs data qubits. We identify the finite interspecies Rydberg-Rydberg interaction strength as a practical obstacle to high-fidelity multi-body entanglement and show that, by tuning the Rabi frequency and the detuning of the Rydberg driving field, the resulting geometric phase error can be compensated. This yields a protocol for simultaneous, non-destructive, in situ stabilizer readout of multiple data qubits via global pulses alone. Using this protocol, we demonstrate non-destructive measurement of Pauli-Z stabilizers on four-qubit Cs plaquettes via a single global Rydberg pulse sequence. Our results demonstrate dual-species tweezer arrays as a promising route towards scalable QEC and open the door to new quantum control protocols leveraging both interspecies and intraspecies interactions.</summary>
  </entry>
  <entry>
    <title>Price and Payoff: Non-Determinism in Fault Tolerant Quantum Computation</title>
    <id>https://arxiv.org/abs/2605.07983</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2605.07983"/>
    <published>2026-05-08T00:00:00Z</published>
    <updated>2026-05-08T00:00:00Z</updated>
<author><name>Aditi Awasthi</name></author><author><name>Sayam Sethi</name></author><author><name>Sahil Khan</name></author><author><name>Gokul Subramanian Ravi</name></author><author><name>Jonathan M. Baker</name></author><category term="error-correction" label="Control for quantum error correction"/>    <summary type="text">A promising approach to achieving scalable fault-tolerant quantum computation is the use of quantum error correction (QEC) codes augmented with magic states i.e. resource states produced via distillation, cultivation, or $R_z$ synthesis and teleported into the circuit as needed. Because magic-state production dominates the space-time volume of fault-tolerant programs, system architects must decide how many production units to allocate. Current approaches rely on deterministic analysis that either provisions for worst-case peak demand (wasting valuable qubit resources on factories that are never simultaneously utilized) or assumes average demand, which increases execution time. In this work, we build a simulation framework that couples circuit scheduling with different stochastic magic state production models, and use it to quantify the impact of non-determinism on circuit execution. We show that non-determinism has a dual effect that deterministic models cannot capture: it inflates total execution time (the price), while deflating peak per-cycle resource demand (the payoff). For distillation-based architectures, this demand smoothing shifts the space-time-optimal provisioning point: fewer factories are needed to minimize space-time volume than deterministic analysis predicts. Across benchmarks, stochastic-aware provisioning reduces space-time volume by up to 27% compared to the deterministic optimum for distillation, while requiring up to 30% fewer factories. We characterize these effects across each preparation mechanism, map the resulting design-space tradeoffs, and demonstrate that static resource estimation systematically mis-characterizes the cost of fault-tolerant execution. Our results establish that stochastic-aware analysis is necessary for right-sizing the factory allocations and should replace deterministic heuristics as the standard methodology for FTQC resource planning.</summary>
  </entry>
  <entry>
    <title>QASM-Eval: A Dataset to Train and Evaluate LLMs on OpenQASM-3 Beyond Quantum Circuits</title>
    <id>https://arxiv.org/abs/2605.30358</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2605.30358"/>
    <published>2026-04-28T00:00:00Z</published>
    <updated>2026-09-25T00:00:00Z</updated>
<author><name>Zhenxiao Fu</name></author><author><name>Lei Jiang</name></author><author><name>Fan Chen</name></author><category term="pulse-level-compilation" label="Pulse-level compilation"/><category term="error-correction" label="Control for quantum error correction"/><category term="dynamical-decoupling" label="Dynamical decoupling"/><category term="machine-learning-control" label="Reinforcement &amp; machine learning for control"/>    <summary type="text">Quantum computing remains in the Noisy Intermediate-Scale Quantum (NISQ) era, with performance constrained by noise. Addressing this limitation requires hardware-facing capabilities beyond gate sequences: mid-circuit measurement and classical feedback for quantum error correction (QEC), precise timing for dynamical decoupling (DD), and pulse-level waveform access for calibration. OpenQASM 3 exposes these capabilities through a hardware-level programming interface. Despite rapid progress in large language models (LLMs) for code generation, datasets targeting these advanced features remain lacking. We introduce QASM-Eval, the first comprehensive dataset to train and evaluate LLMs on OpenQASM 3, targeting completion of hardware-facing constructs within a supplied program context. QASM-Eval comprises an expert-curated test set of 1,200 tasks and a training set of over 4,000 tasks, covering classical logic, timing scheduling, pulse control, and complex tasks inspired by quantum-control workflows. An extended verifier automatically checks syntax, quantum measurement distributions, and program timelines. Our evaluation identifies substantial headroom for OpenQASM 3 code generation and significant gains from targeted fine-tuning. Fine-tuned Llama-3-8B outperforms zero-shot GPT-5.6-Terra, while fine-tuned Llama-3-70B achieves 61.17% overall pass@1 and approaches few-shot-augmented GPT-5.6-Terra. QASM-Eval provides a benchmark and training resource for specification-guided code generation over the hardware-facing constructs of OpenQASM 3, supporting the development of LLM assistants for quantum programming. Data and code: https://github.com/fuzhenxiao/QASM-Eval</summary>
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