<?xml version="1.0" encoding="utf-8"?><feed xmlns="http://www.w3.org/2005/Atom">
  <title>QOC — Pulse-level compilation</title>
  <subtitle>Quantum control papers on arXiv, selected and classified automatically by QOC.</subtitle>
  <id>https://llorebaga.github.io/QOC/topics/pulse-level-compilation/</id>
<link rel="alternate" type="text/html" href="https://llorebaga.github.io/QOC/topics/pulse-level-compilation/"/>
  <link rel="self" type="application/atom+xml" href="https://llorebaga.github.io/QOC/topics/pulse-level-compilation/feed.xml"/>  <updated>2026-10-15T00:00:00Z</updated>
  <generator>QOC</generator>
  <entry>
    <title>Quantum control of solid state qubits via Reinforcement Learning</title>
    <id>https://arxiv.org/abs/2610.21987</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2610.21987"/>
    <published>2026-10-15T00:00:00Z</published>
    <updated>2026-10-15T00:00:00Z</updated>
<author><name>Dennis Herb</name></author><author><name>Mirko Rossini</name></author><author><name>Sabine Wölk</name></author><author><name>Joachim Ankerhold</name></author><author><name>Dominik Maile</name></author><author><name>Alessio Belenchia</name></author><category term="gate-synthesis" label="Quantum gate synthesis"/><category term="machine-learning-control" label="Reinforcement &amp; machine learning for control"/><category term="pulse-level-compilation" label="Pulse-level compilation"/><category term="spins" label="Spins — NMR, ESR &amp; colour centres"/>    <summary type="text">The use of reinforcement learning (RL) in the design of quantum control strategies for pulse level control of NISQ era quantum devices is attracting growing interest. Model-free RL, not requiring preexisting knowledge of the physical system, acts as a black-box optimization tool well suited for noisy devices. In this work, we provide a simulation-based analysis of the performance of model-free RL for state preparation and qubit gate design in a challenging setup: indirect control of NV nuclear spins in a spin-bath. In particular, the spin-bath is modeled via the generalized cluster correlation expansion accounting for magnetic impurities and intra-bath interactions. We analyze the performance of the RL agents by performing simulations with minimally observable environments and noisy, sparse rewards as introduced in (Phys. Rev. X 12, 011059), and compare them to other state-of-the-art black-box optimization tools.</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>Design-Time Conformance Checking for Pulse-Level Quantum Control</title>
    <id>https://arxiv.org/abs/2610.10427</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2610.10427"/>
    <published>2026-10-07T00:00:00Z</published>
    <updated>2026-10-07T00:00:00Z</updated>
<author><name>Rylan Malarchick</name></author><category term="pulse-level-compilation" label="Pulse-level compilation"/>    <summary type="text">A pulse-level quantum control program is written against a device whose limits are recorded, if at all, in vendor documentation and source code. A program that exceeds them can be refused at compile time. It can also be accepted and silently altered, or compile and then fail at the board. In the last two cases the experiment runs, and the data does not correspond to the program that was written. We present qconform, a checker that decides whether a pulse program is realizable on a device, given a versioned capability descriptor for that device. Every constraint in a descriptor cites the toolchain observation that established it. The checker is design-time, offline, and deterministic, and it uses no floating point. It reports a verdict, the rules it applied, and a coverage manifest that names what it did not check. We evaluate qconform by differential testing against the QICK and Qblox toolchains, on three QICK board configurations and one Qblox cluster. Over 1263 program runs of 969 distinct programs, the checker accepted no program that a toolchain refuses. On both vendors, a descriptor pinned to one toolchain release accepts programs that older releases refuse. The evaluation also found ten defects in the checker and its descriptors, all fixed.</summary>
  </entry>
  <entry>
    <title>JAQSI: Just Another Quantum Simulator</title>
    <id>https://arxiv.org/abs/2610.05086</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2610.05086"/>
    <published>2026-10-04T00:00:00Z</published>
    <updated>2026-10-04T00:00:00Z</updated>
<author><name>Melvin Strobl</name></author><author><name>Maja Franz</name></author><author><name>Lukas Scheller</name></author><author><name>Eileen Kuehn</name></author><author><name>Wolfgang Mauerer</name></author><author><name>Achim Streit</name></author><category term="pulse-level-compilation" label="Pulse-level compilation"/><category term="autodiff-control" label="Automatic differentiation &amp; differentiable programming"/><category term="many-body-control" label="Many-body optimal control"/>    <summary type="text">Classical simulation supports the development and validation of quantum algorithms through full-state inspection, controlled noise models and backpropagation, albeit for small quantum systems. Existing frameworks offer gate-level execution, differentiable pulse-level dynamics or optimised hardware execution. Just another quantum simulator (JAQSI) combines gate- and pulse-level simulation in one differentiable circuit model built upon JAX. Circuits are represented as pure functions of numerical inputs which support vectorised batches and JIT compilation. Within a single circuit, matrix-defined operations, gates synthesised from Hamiltonian time evolution and noise channels can be composed freely. For a fast simulation, gate and channel fusion reduces passes over the state, while adjoint differentiation computes expectation-value gradients with a constant number of statevectors. At pulse level, JAQSI reduces evolution under single-term Hamiltonians to a scalar pulse-area integral and reuses cached execution plans and compiled solvers. In a benchmark we compare JAQSI with PennyLane, Qiskit, Qibo, Qulacs, QuTiP and dynamiqs. At gate level, we observe performance either on par or an order of magnitude faster across statevector, density, noise and gradient simulation than the compared simulators up to 12 qubits. Beyond 18 qubits, JAQSI is on par with PennyLane Lightning in both statevector and gradient simulation. In the statevector and noisy density-matrix pulse benchmarks, it is at least 5 times faster than the other simulators, even with its closed-form solve disabled. Disabling the latter increases its runtime by at most a factor of 1.5. We provide JAQSI as open-source software on GitHub and PyPI.</summary>
  </entry>
  <entry>
    <title>Pulse-resolved post-generation phase control of squeezed light at 93 MHz with a bulk lithium-niobate modulator</title>
    <id>https://arxiv.org/abs/2610.03257</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2610.03257"/>
    <published>2026-10-02T00:00:00Z</published>
    <updated>2026-10-02T00:00:00Z</updated>
<author><name>Edoardo Suerra</name></author><author><name>Igor Vasiljevic</name></author><author><name>Sebastiano Corli</name></author><author><name>Enrico Prati</name></author><author><name>Simone Cialdi</name></author><category term="photonics" label="Photonic &amp; optomechanical systems"/><category term="bosonic-control" label="Bosonic &amp; continuous-variable control"/><category term="pulse-level-compilation" label="Pulse-level compilation"/>    <summary type="text">Time-domain multiplexing of continuous-variable quantum states provides a scalable approach to photonic quantum information processing, in which individual temporal modes can be sequentially manipulated within a common optical path. Here we demonstrate pulse-resolved post-generation phase control of squeezed-vacuum states at a repetition rate of 93 MHz using a low-loss bulk lithium-niobate electro-optic modulator driven by a broadband RF power amplifier. The driving architecture exploits low-cost, commercially available RF components and the impedance mismatch between the RF chain and the capacitive crystal load, rather than relying on dedicated custom high-voltage electronics, to obtain large voltage excursions on the modulator while operating above the piezoelectric-resonance region of lithium niobate. The modulator is driven synchronously with the optical pulse train, enabling the phase of consecutive temporal modes to be individually controlled. An interferometric calibration yields a maximum differential phase excursion of 1.93 rad. We apply the modulator to a 1035 nm squeezed-vacuum field generated by a synchronously pumped optical parametric oscillator and characterize the output using time-resolved balanced homodyne detection. With the local-oscillator phase kept fixed, the phase of the squeezed state is varied from pulse to pulse, and the corresponding phase-dependent quadrature variance is reconstructed. The resulting quadrature scan agrees with an equivalent measurement obtained by varying the local-oscillator phase with a piezoelectric actuator. These results demonstrate post-generation quantum-state phase control at the individual-pulse level and provide an electro-optic building block for programmable manipulation of time-multiplexed quantum states in recirculating optical architectures.</summary>
  </entry>
  <entry>
    <title>Distinguishing Coherent Crosstalk from Calibration Drift via Pauli-Transfer Signatures and Quantum Edge Detection</title>
    <id>https://arxiv.org/abs/2609.40283</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2609.40283"/>
    <published>2026-09-30T00:00:00Z</published>
    <updated>2026-09-30T00:00:00Z</updated>
<author><name>Syed Emad Uddin Shubha</name></author><author><name>Tasnuva Farheen</name></author><category term="pulse-level-compilation" label="Pulse-level compilation"/><category term="closed-loop" label="Closed-loop &amp; in-situ optimization"/><category term="gate-synthesis" label="Quantum gate synthesis"/>    <summary type="text">Multi-tenant quantum processors expose a pulse-level attack surface in which coherent crosstalk can mimic benign calibration drift at matched average gate infidelity. We present a structural verification and detection framework based on the residual Pauli transfer matrix (PTM). We prove that products of local unital, trace-preserving channels cannot mix weight-1 and weight-2 Pauli operators, even under coherent drift of arbitrary strength or axis. Building on established PTM-to-Hamiltonian relations, we prove that, for any specified qubit pair in an arbitrarily large system, the first-order map from its nine interaction coefficients to the antisymmetric cross-weight feature is an isometry up to scale. Thus, every interaction direction is locally observable near the identity. We also exhibit cancellation of this feature under large local rotations and prove that the full cross-weight norm is invariant under local unitary composition, providing a structural countermeasure. For calibrated small local rotations, shared randomized-Pauli measurements support periodic verification using the evaluated antisymmetric detector. In simulation, $16{,}384$ randomized settings yield a detection threshold of $λ_{\min}\approx0.13$ at a $5\%$ calibrated false-positive target, with approximately $M^{-1/2}$ scaling in the number of settings $M$. Further experiments characterize detection under relaxation, depolarization, native ZZ fluctuations, and time-dependent pulse dynamics. Finally, an FRQI encoding with Pauli-graph quantum Hadamard edge detection reproduces the classical structural edge score to numerical precision.</summary>
  </entry>
  <entry>
    <title>Gate Synthesis in Dephasing-Limited Nitrogen-Vacancy Ensembles</title>
    <id>https://arxiv.org/abs/2609.31913</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2609.31913"/>
    <published>2026-09-25T00:00:00Z</published>
    <updated>2026-09-25T00:00:00Z</updated>
<author><name>Ankita Chakravarty</name></author><author><name>Arnaud Carignan-Dugas</name></author><author><name>Eva Dupont-Ferrier</name></author><author><name>Yves Bérubé-Lauzière</name></author><category term="spins" label="Spins — NMR, ESR &amp; colour centres"/><category term="composite-pulses" label="Composite pulses"/><category term="quantum-sensing" label="Control for sensing &amp; metrology"/><category term="pulse-level-compilation" label="Pulse-level compilation"/>    <summary type="text">Ensemble nitrogen-vacancy (NV) centers are widely used for quantum sensing and magnetometry, where performance depends on the accurate implementation of microwave pulse sequences. In these systems, inhomogeneous broadening and short coherence times limit reliable multi-pulse control, while hardware imperfections and off-resonant excitation distort implemented rotations, making direct calibration of arbitrary gates tedious. To address this, we implement a control framework with a ZXZXZ gate decomposition which uses fixed-angle, phase-parameterized pulses, enabling universal single-qubit control from a single calibrated $ π/2$ primitive ($X_{π/2}$) along with virtual Z operations. We compare a standard pulse with a composite pulse designed for high-power operation in a regime where the Rabi frequency is comparable to the hyperfine splitting, leading to non-uniform evolution across hyperfine levels. Using pre-determined combinations of $π/2$ pulse sequences, we observe that standard pulses rapidly deviate from ideal behavior under repeated application, while the composite pulse suppresses this error accumulation by more than 70$\%$ for longer sequences despite its longer duration. In contrast, randomized benchmarking yields similar decay factors for both implementations, highlighting its limited sensitivity to coherent control errors. These results establish a practical route to robust control in short-coherence ensemble systems and emphasize the importance of pulse-level characterization.</summary>
  </entry>
  <entry>
    <title>Counterdiabatic quantum optimization for efficient state preparation in the Schwinger model</title>
    <id>https://arxiv.org/abs/2609.31400</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2609.31400"/>
    <published>2026-09-25T00:00:00Z</published>
    <updated>2026-09-25T00:00:00Z</updated>
<author><name>Ethan Laval</name></author><author><name>Bipasha Chakraborty</name></author><author><name>Stefano Cipolla</name></author><category term="variational-algorithms" label="Variational algorithms &amp; QAOA as control"/><category term="state-preparation" label="State preparation &amp; transfer"/><category term="shortcuts-to-adiabaticity" label="Shortcuts to adiabaticity"/><category term="pulse-level-compilation" label="Pulse-level compilation"/>    <summary type="text">The Quantum Approximate Optimization Algorithm (QAOA), whose design is underpinned by the adiabatic theorem, is one of the leading variational quantum algorithms for preparing the ground states of gauge theories. A recently proposed variant, DC-QAOA, incorporates counterdiabatic driving to accelerate the adiabatic process, reducing both circuit depth and runtime. In this work, we present a systematic analysis, from both theoretical and computational perspectives, of DC-QAOA and related counterdiabatic variants for preparing the ground state of the Schwinger model, the paradigmatic (1+1)-dimensional lattice gauge theory. Benchmarking these methods against standard QAOA, we show that counterdiabatic driving improves ground-state preparation while lowering circuit depth requirements. Our results establish counterdiabatic protocols as a practical route towards efficient quantum simulation of gauge theories.</summary>
  </entry>
  <entry>
    <title>Trading Circuit Depth for Pulse Sparsity in Chromatic Dynamical Decoupling</title>
    <id>https://arxiv.org/abs/2609.30175</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2609.30175"/>
    <published>2026-09-24T00:00:00Z</published>
    <updated>2026-09-24T00:00:00Z</updated>
<author><name>Amy F. Brown</name></author><author><name>Daniel A. Lidar</name></author><category term="dynamical-decoupling" label="Dynamical decoupling"/><category term="pulse-level-compilation" label="Pulse-level compilation"/>    <summary type="text">Suppressing decoherence and crosstalk systematically across large networks of qubits is a pressing concern as qubit counts increase rapidly. General multi-qubit dynamical decoupling (DD) has historically been based on Hadamard matrices and orthogonal arrays, with instantaneous-pulse sequences whose circuit depth scales linearly with the number of qubits. Chromatic-Hadamard DD (CHaDD) improves upon these methods by properly coloring the hardware graph and assigning to each color a row of a Hadamard matrix, resulting in a circuit depth that scales linearly with the number of colors $C$, which can be as low as the chromatic number of the graph. Here, we explore the tradeoff between circuit depth and the pulse repetition rate (PRR), the average fraction of time steps in which a qubit is pulsed, i.e., a measure of pulse density. We introduce two single-axis sequences based on binary and Gray matrices, Chromatic-Binary DD (CBDD) and Chromatic-Gray DD (CGDD), which, for $C&gt;2$, are special cases of non-minimum-depth CHaDD and achieve PRR $&lt;2/C$ and PRR $=1/C$, respectively, compared with a PRR above $1/4$ for CHaDD, at the price of a circuit depth of $2^C$. In state preservation experiments on a $127$-qubit IBM processor with $C=3$, the less dense sequences outperform CHaDD at short times when the pulses are not robust; this advantage is largely eliminated by robust versions designed to compensate for coherent pulse errors, and among the robust sequences, CGDD uses the fewest pulses over a fixed protection time. Across non-robust $C=3$ and $C=5$ schedules, equal PRR on a fixed qubit subset is empirically associated with similar state preservation. Thus, the PRR serves as a practical figure of merit for chromatic DD whenever coherent pulse errors dominate.</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>Adaptive AI for Pulse-Level Quantum Control</title>
    <id>https://arxiv.org/abs/2609.08727</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2609.08727"/>
    <published>2026-09-08T00:00:00Z</published>
    <updated>2026-09-08T00:00:00Z</updated>
<author><name>Sanjeev Shapkota</name></author><author><name>Yayu Mo</name></author><author><name>Sanjaya Lohani</name></author><category term="pulse-level-compilation" label="Pulse-level compilation"/><category term="superconducting" label="Superconducting circuits"/><category term="variational-algorithms" label="Variational algorithms &amp; QAOA as control"/><category term="machine-learning-control" label="Reinforcement &amp; machine learning for control"/>    <summary type="text">The Control Variational Quantum Eigensolver (ctrl-VQE) directly optimizes microwave pulses to enable faster and lower-error quantum-state preparation, but its continuous control landscape re- quires efficient search strategies. We demonstrate that a reinforcement-learning agent based on a deep Q learning network can autonomously discover high-performance pulse sequences using only system parameters and a reward function. The approach is fully general for superconducting qubit platforms, requires no ansatz, and operates at nanosecond resolution compatible with hardware con- straints. As a proof of concept, we apply the method to ground-state preparation of the Hydrogen molecule on a simulated superconducting device. The agent consistently identifies optimized control sequences that achieve high fidelity and outperform random-search baselines. These results highlight adaptive learning as a promising hardware-ready framework for pulse-level quantum control.</summary>
  </entry>
  <entry>
    <title>Shuttling-aware dynamical decoupling for quantum charge-coupled devices</title>
    <id>https://arxiv.org/abs/2609.03014</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2609.03014"/>
    <published>2026-09-02T00:00:00Z</published>
    <updated>2026-09-02T00:00:00Z</updated>
<author><name>Linus Schulte</name></author><author><name>Aaron Sander</name></author><author><name>Robert Wille</name></author><category term="dynamical-decoupling" label="Dynamical decoupling"/><category term="pulse-level-compilation" label="Pulse-level compilation"/>    <summary type="text">Dynamical decoupling (DD) helps maintain high-fidelity quantum computations by suppressing dephasing noise through carefully timed refocusing pulses. In quantum charge-coupled device (QCCD) architectures, however, where ions are shuttled throughout the device, transport constrains when pulses can be applied and affects the phase accumulated by an ion. Conventional DD methods do not account for shuttling and may therefore schedule pulses that must be omitted or shifted after transport scheduling, weakening the protection from dephasing. We therefore introduce shuttling-aware dynamical decoupling (SADD), an offline compiler pass that jointly selects refocusing pulses and local ion rerouting while preserving logical-gate timings and the total schedule length. In benchmark simulations, SADD improves average final-state fidelity over both the original schedules and a simple nearest-feasible Hahn-echo baseline when dephasing dominates control and transport errors and varies slowly enough for DD. Rerouting enables otherwise infeasible pulse timings, while spatial information about the noise can provide further gains. These benefits disappear, however, when the added transport introduces too much error. Overall, our results show that coordinating DD with ion transport is an effective compiler strategy for reducing dephasing in QCCD processors.</summary>
  </entry>
  <entry>
    <title>Hardware-Efficient Error Mitigation and Shot-Efficient Sampling on IBM Quantum Hardware</title>
    <id>https://arxiv.org/abs/2608.28535</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2608.28535"/>
    <published>2026-08-28T00:00:00Z</published>
    <updated>2026-08-28T00:00:00Z</updated>
<author><name>Sumit Chongder</name></author><category term="dynamical-decoupling" label="Dynamical decoupling"/><category term="pulse-level-compilation" label="Pulse-level compilation"/>    <summary type="text">We experimentally study error mitigation and finite-shot sampling on superconducting quantum hardware under a constrained execution budget. The study combines calibration-aware qubit selection, circuit-depth scaling, zero-noise extrapolation, dynamical decoupling, readout-error mitigation, and repeated-shot estimation on an IBM Quantum processor. Experiments are organized across ideal simulation, noise-model simulation, and physical-device execution to separate sampling uncertainty from device-induced error. We investigate how mitigation performance changes with circuit depth, effective noise scale, qubit connectivity, and measurement budget, and quantify accuracy using expectation-value error, mean-squared error, statistical uncertainty, and mitigation gain. A fixed hardware-execution budget is used to evaluate shot allocation strategies and repeated measurements without relying on unlimited sampling. The resulting analysis provides a hardware-aware characterization of when mitigation improves expectation-value estimation and when finite-shot fluctuations offset the benefit of additional mitigation overhead. The implementation uses contemporary Qiskit and IBM Quantum Runtime workflows and is designed to provide reproducible experimental evidence for error-mitigation studies on current quantum processors.</summary>
  </entry>
  <entry>
    <title>Verification Meets Calibration: Bounds and Secret-Independent State Preparation with an NV-Center as a Case Study</title>
    <id>https://arxiv.org/abs/2609.20219</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2609.20219"/>
    <published>2026-08-19T00:00:00Z</published>
    <updated>2026-08-19T00:00:00Z</updated>
<author><name>Ezra Acalapati</name></author><author><name>Elham Kashefi</name></author><author><name>Cica Gustiani</name></author><category term="spins" label="Spins — NMR, ESR &amp; colour centres"/><category term="pulse-level-compilation" label="Pulse-level compilation"/><category term="state-preparation" label="State preparation &amp; transfer"/><category term="closed-loop" label="Closed-loop &amp; in-situ optimization"/>    <summary type="text">Verification protocols provide cryptographic guarantees that the outcome of a delegated quantum computation is correct, a key requirement for scalable and trustworthy quantum computing. A central assumption underlying these protocols is secret independence: the noise affecting state preparation must not depend on the classical secrets that specify the prepared states. In earlier protocols this assumption was enforced by the physical separation of client and server; in the recent on-chip setting it becomes a property of the hardware itself, and one that high-fidelity devices do not automatically satisfy. We first make the requirement quantitative, deriving a bound that shows how residual secret dependence limits the size of any verifiable computation within this framework. Motivated by this, we introduce a calibration framework that enforces secret independence through pulse-level quantum control, producing state preparations that are simultaneously high-fidelity and secret-independent. We assess its performance on a nitrogen-vacancy centre system via emulation, showing that it reduces the secret dependence of the preparations by more than an order of magnitude compared to standard optimal control, and that it is robust against detuning and drive-amplitude errors commonly encountered in experiment. The framework operates entirely at the calibration stage and is platform-agnostic, offering a practical pathway towards verifiable quantum computing at scale.</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>Motional refocusing for trap-off Rydberg gates</title>
    <id>https://arxiv.org/abs/2608.04812</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2608.04812"/>
    <published>2026-08-05T00:00:00Z</published>
    <updated>2026-08-05T00:00:00Z</updated>
<author><name>Yoav Sagi</name></author><author><name>Ofer Firstenberg</name></author><author><name>Nir Davidson</name></author><author><name>Guy Raz</name></author><category term="neutral-atoms" label="Neutral atoms &amp; Rydberg arrays"/><category term="drag" label="DRAG &amp; leakage suppression"/><category term="dynamical-decoupling" label="Dynamical decoupling"/><category term="pulse-level-compilation" label="Pulse-level compilation"/>    <summary type="text">Rydberg entangling gates in optical-tweezer arrays are commonly executed with the trapping light switched off, so every gate contains a release--and--recapture cycle that heats the atomic motion and can ultimately limit circuit depth. We develop a motional refocusing protocol that exactly removes this heating in the harmonic approximation using only programmable intensity switching of the trapping light. The protocol closes the release--and--recapture cycle for every matched harmonic mode, returning arbitrary motional populations and coherences exactly up to ordinary evolution under the static trap. We derive the recovery sequence in closed form for arbitrary catch depth and prove that, within the experimentally relevant regime, it is the unique globally time-optimal solution under bounded trap intensity. The harmonic theory is then extended in two directions. First, we construct exact common-intensity recovery sequences that simultaneously refocus several nondegenerate harmonic modes, including radial--axial and fully anisotropic three-dimensional traps. Second, we derive a composite sequence that suppresses the leading anharmonic correction of weakly anharmonic traps by canceling all first-order motional transitions induced by the quartic anharmonicity, changing the residual heating law from $U_0^{-2}$ to $U_0^{-4}$. Wave-packet simulations in realistic Gaussian tweezers validate the analytic theory and quantify the residual effects of anharmonicity, finite switching ramps, trap ellipticity, and control errors. Applied to representative cesium Rydberg gates, the protocol suppresses the dominant recapture heating to the anharmonic floor and prevents the associated motional Doppler contribution from increasing with circuit depth. The resulting framework provides a practical route toward heating-free trap-off neutral-atom gates using only trap-intensity modulation.</summary>
  </entry>
  <entry>
    <title>Analytic gradients for low-rank quantum optimal control</title>
    <id>https://arxiv.org/abs/2607.14217</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2607.14217"/>
    <published>2026-07-15T00:00:00Z</published>
    <updated>2026-07-15T00:00:00Z</updated>
<author><name>Leo Goutte</name></author><author><name>Vincenzo Savona</name></author><category term="superconducting" label="Superconducting circuits"/><category term="open-system-control" label="Control of open quantum systems"/><category term="pulse-level-compilation" label="Pulse-level compilation"/><category term="state-preparation" label="State preparation &amp; transfer"/>    <summary type="text">We introduce low-rank optimal control (LROC), a method for designing control pulses in open quantum systems whose full density-matrix simulation is prohibitively expensive. The method exploits a feature of quantum computing itself: because protocols are designed to preserve purity, the density matrix is dominated by a few pure states and admits an accurate low-rank factorization. LROC propagates only this factorized form and, by deriving the corresponding adjoint equation, obtains the gradient of any differentiable objective at the same reduced cost as the simulation, leading to a quadratic improvement in time and memory compared to the full master equation. We illustrate the breadth of the method on four superconducting-circuit tasks: preparation of a five-qubit GHZ state, a CNOT gate, qubit readout, and an error correction primitive, modeled with realistic multilevel transmons, decay, and strong drives, in each case reaching fidelities consistent with the intrinsic dissipation limits. LROC thereby extends pulse-level optimization to system sizes beyond the reach of existing gradient-based methods.</summary>
  </entry>
  <entry>
    <title>Branch-resolved Pauli-block spectroscopy of residual conditional phase in two-qubit gates</title>
    <id>https://arxiv.org/abs/2607.10249</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2607.10249"/>
    <published>2026-07-11T00:00:00Z</published>
    <updated>2026-07-15T00:00:00Z</updated>
<author><name>Xudan Chai</name></author><author><name>Yanwu Gu</name></author><author><name>Huiqi Xue</name></author><author><name>Kerui Li</name></author><author><name>Dong E. Liu</name></author><category term="gate-synthesis" label="Quantum gate synthesis"/><category term="closed-loop" label="Closed-loop &amp; in-situ optimization"/><category term="pulse-level-compilation" label="Pulse-level compilation"/>    <summary type="text">Recent progress in quantum physics and quantum technologies is driving quantum computing from the noisy intermediate-scale (NISQ) era toward fault-tolerant operation. High-precision control of two-qubit gates is among the most critical requirements in this transition and hinges on accurate two-qubit calibration. For controlled-phase and CZ-style operations, the residual conditional phase (the nonlocal ZZ-type deviation after local compensation) is weakly resolved at leading order in average infidelity and randomized benchmarking, and repeated Ramsey amplification does not reliably isolate it from ordinary target detuning, SPAM errors, and contrast loss in long sequences. We introduce branch-resolved Pauli-block spectroscopy to estimate the per-cycle residual ZZ-rotation angle theta_c with its sign, from which the controlled-phase residual follows by a fixed convention. The protocol repeats a fixed probe for N cycles, measures the closed Pauli block IX, IY, ZX, and ZY, and forms branch coherences C+ and C- conditioned on the control qubit; theta_c splits the two branch phase slopes in opposite directions, while local target phase beta_c shifts them together. An echoed-cycle variant suppresses removable local terms while preserving the nonlocal contribution. Numerical simulations with injected theta_c, detuning, damping, and SPAM confirm unbiased signed readout where scalar-sector alternatives fail and distinguish opposite-sign errors at equal infidelity. On one superconducting cloud qubit-coupler pair, a pulse-level calibration closed loop shows near-linear injection, preserved branch contrast, and tracking of the native residual conditional phase through one iteration. The approach yields a low-overhead, signed per-cycle estimate of residual conditional phase that standard fidelity benchmarks underresolve at leading order.</summary>
  </entry>
  <entry>
    <title>Vectorizing Quantum Control: A RISC-V Vector Extension Architecture for Scalable Qubit Systems</title>
    <id>https://arxiv.org/abs/2607.07372</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2607.07372"/>
    <published>2026-07-08T00:00:00Z</published>
    <updated>2026-08-18T00:00:00Z</updated>
<author><name>Xiaorang Guo</name></author><author><name>Kun Qin</name></author><author><name>Yanbin Chen</name></author><author><name>Carsten Trinitis</name></author><author><name>Martin Schulz</name></author><category term="pulse-level-compilation" label="Pulse-level compilation"/><category term="control-hardware" label="Control electronics &amp; software stacks"/><category term="feedback-control" label="Measurement-based feedback"/>    <summary type="text">The Quantum Control Processor (QCP) bridges the gap between compiler toolchains and control electronics, and is responsible for translating compiled quantum circuits into executable instructions that directly manipulate qubits and handle measurement feedback. However, existing designs rely primarily on customized instruction sets, limiting design reuse and requiring significant effort to build supporting toolchains. Furthermore, efficiently addressing qubits and scheduling operations in highly scalable scenarios remains a critical challenge. In this work, we present a vectorized quantum control approach built upon the RISC-V Vector (RVV) engine with a quantum-oriented extension. Leveraging the high parallelism of RVV, our approach can address up to 128 qubits in a single instruction. We also embed parameterized rotation information into the instruction set, enabling dynamic tuning of gate rotations in hybrid quantum-classical programs. To support mid-circuit measurements, we design a hardware-based halt-resume protocol that resumes pipeline execution within 80 $ns$ of receiving the measurement result. Comprehensive evaluation using both RISC-V toolchains and FPGA prototypes demonstrates that our design achieves up to 2.52$\times$ speedup over the baseline in program execution time, with excellent scalability.</summary>
  </entry>
  <entry>
    <title>Synthesizing Compound Pulse Gadgets for Hamiltonian Simulation on Trapped-Ion Platforms</title>
    <id>https://arxiv.org/abs/2607.00826</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2607.00826"/>
    <published>2026-07-01T00:00:00Z</published>
    <updated>2026-07-01T00:00:00Z</updated>
<author><name>Ria Patel</name></author><author><name>Masoud Hakimi Heris</name></author><author><name>Yuan Liu</name></author><author><name>Frank Mueller</name></author><category term="pulse-level-compilation" label="Pulse-level compilation"/><category term="trapped-ions" label="Trapped ions"/><category term="grape" label="GRAPE"/><category term="open-system-control" label="Control of open quantum systems"/>    <summary type="text">Standard gate-level transpilation introduces significant physical noise and overhead for high-precision quantum algorithms, such as the Quantum Singular Value Transformation (QSVT), on near-term trapped-ion hardware. Current compilers treat quantum operations as discrete units, forcing the physical control layer to execute highly fragmented laser pulses. To address this hardware-software disconnect, this work introduces a holistic pulse synthesis strategy that bypasses discrete gate-stitching to compile algorithms directly into continuous compound pulse gadgets. As a proof-of-concept, we target Hamiltonian simulation of the $H_2$ molecule, block-encoding the problem into a QSVT circuit to approximate the time-evolution operator $U = e^{-i H t}$ across 3 computational ions (2 system, 1 ancilla). We utilize the Gradient Ascent Pulse Engineering (GRAPE) algorithm to generate these compound gadgets and evaluate our methodology using noisy Lindblad master equation simulations. Preliminary observations indicate that the proposed strategy achieves significant temporal compression, reducing the total pulse schedule duration compared to standard compilers. Furthermore, synthesizing operations holistically eliminates the control-layer latency associated with discrete pulse lookup overhead. By streamlining the physical control schedule, this methodology offers a promising pathway to execute operations faster, highlighting the potential for compound gadgets to increase the computational depth achievable within fundamental $T_2$ decoherence limits.</summary>
  </entry>
  <entry>
    <title>Quantum simulation of neutrino oscillations with bosonic encoding</title>
    <id>https://arxiv.org/abs/2606.18755</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2606.18755"/>
    <published>2026-06-17T00:00:00Z</published>
    <updated>2026-06-17T00:00:00Z</updated>
<author><name>Sandeep Joshi</name></author><category term="bosonic-control" label="Bosonic &amp; continuous-variable control"/><category term="superconducting" label="Superconducting circuits"/><category term="gate-synthesis" label="Quantum gate synthesis"/><category term="pulse-level-compilation" label="Pulse-level compilation"/>    <summary type="text">Superconducting qubits offer a versatile platform for quantum simulation. In this architecture, quantum information can be encoded in the bosonic modes of a microwave cavity, offering an alternative to conventional qubit-based encoding schemes. These cavity bosonic modes can be manipulated using a single ancillary qubit. In this work, we investigate the quantum simulation of two- and three-flavor neutrino oscillations using Fock-basis encoding of a cavity mode. We design pulse sequences for implementing the required unitary operations through selective number-dependent arbitrary phase (SNAP) and displacement gates. Pulse-level control is employed to realize high-fidelity gate operations on the encoded cavity mode. The resulting neutrino oscillation probabilities obtained from quantum simulation exhibit close agreement with the corresponding theoretical predictions, demonstrating the feasibility of cavity-based bosonic encoding schemes for quantum simulation.</summary>
  </entry>
  <entry>
    <title>Noise-Adaptive Predictive Dynamical Decoupling</title>
    <id>https://arxiv.org/abs/2606.15769</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2606.15769"/>
    <published>2026-06-14T00:00:00Z</published>
    <updated>2026-06-14T00:00:00Z</updated>
<author><name>Ali Abu-Nada</name></author><author><name>Subhashish Banerjee</name></author><author><name>Lian-Ao Wu</name></author><category term="dynamical-decoupling" label="Dynamical decoupling"/><category term="open-system-control" label="Control of open quantum systems"/><category term="machine-learning-control" label="Reinforcement &amp; machine learning for control"/><category term="pulse-level-compilation" label="Pulse-level compilation"/>    <summary type="text">Protecting quantum coherence against realistic environmental noise remains one of the fundamental obstacles to scalable quantum technologies. We develop a noise-adaptive dynamical decoupling framework that combines analytical open-quantum-system modeling with machine-learning-based forecasting for a qubit interacting with random telegraph noise. Unlike conventional dynamical decoupling protocols based on fixed pulse schedules, the proposed approach continuously forecasts short-time coherence evolution and adaptively applies control pulses according to the instantaneous noise dynamics. We investigate stationary and non-stationary environments spanning both Markovian and non-Markovian regimes. Numerical simulations demonstrate that the machine-learning-assisted adaptive control strategy substantially outperforms conventional periodic dynamical decoupling while using a comparable number of control pulses. The improvement becomes particularly pronounced in non-Markovian and non-stationary regimes, where memory effects, coherence revivals, and temporally evolving noise strongly limit the effectiveness of static pulse protocols. These results establish predictive machine-learning-assisted dynamical decoupling as a promising and scalable framework for adaptive quantum control in realistic noisy quantum devices.</summary>
  </entry>
  <entry>
    <title>QuBE/Qubex: an integrated hardware-software system for superconducting qubit experiments with broadband control</title>
    <id>https://arxiv.org/abs/2606.13010</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2606.13010"/>
    <published>2026-06-11T00:00:00Z</published>
    <updated>2026-06-11T00:00:00Z</updated>
<author><name>Akinori Machino</name></author><author><name>Kazuhisa Ogawa</name></author><author><name>Takefumi Miyoshi</name></author><author><name>Hidehisa Shiomi</name></author><author><name>Shinichi Morisaka</name></author><author><name>Ryo Matsuda</name></author><author><name>Nilton F. G. Filho</name></author><author><name>Koichiro Ban</name></author><author><name>Takafumi Miyanaga</name></author><author><name>Keisuke Koike</name></author><author><name>Ryutaro Ohira</name></author><author><name>Toshi Sumida</name></author><author><name>Yoshinori Kurimoto</name></author><author><name>Yuuya Sugita</name></author><author><name>Yosuke Ito</name></author><author><name>Yasunari Suzuki</name></author><author><name>Peter A. Spring</name></author><author><name>Shiyu Wang</name></author><author><name>Hiroto Mukai</name></author><author><name>Arvind Mamgain</name></author><author><name>Shuhei Tamate</name></author><author><name>Yutaka Tabuchi</name></author><author><name>Yasunobu Nakamura</name></author><author><name>Makoto Negoro</name></author><category term="superconducting" label="Superconducting circuits"/><category term="gate-synthesis" label="Quantum gate synthesis"/><category term="pulse-level-compilation" label="Pulse-level compilation"/><category term="closed-loop" label="Closed-loop &amp; in-situ optimization"/>    <summary type="text">Achieving high-fidelity operation in large-scale superconducting qubit systems requires not only control hardware with broad frequency coverage, low crosstalk, and tight synchronization but also software that coordinates system configuration, experiment execution, and data analysis. Here we present an integrated qubit-control system that combines broadband microwave hardware with a pulse-level software stack for scalable superconducting qubit experiments. The hardware provides broadband microwave coverage, including an instantaneous span of up to 1.6 GHz from a control output, while the software reduces setup and calibration overhead through automated configuration and built-in experiment workflows. We validate the system on a 64-qubit fixed-frequency transmon chip through full-chip frequency identification and representative demonstrations, including multi-unit far-detuned cross-resonance calibration and benchmarking that yields a measured two-qubit gate fidelity of 98.34%, and multilevel readout beyond the computational subspace. By disclosing the hardware architecture and releasing the software stack as open source, this work provides an inspectable hardware-software foundation for scalable superconducting qubit control experiments.</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>Continuous-time quantum control across an exponentially small bottleneck in a frustrated Ising ring model</title>
    <id>https://arxiv.org/abs/2606.07168</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2606.07168"/>
    <published>2026-06-05T00:00:00Z</published>
    <updated>2026-06-05T00:00:00Z</updated>
<author><name>Vincenzo Roberto Arezzo</name></author><author><name>Kiran Thengil</name></author><author><name>Giuseppe Santoro</name></author><category term="variational-algorithms" label="Variational algorithms &amp; QAOA as control"/><category term="state-preparation" label="State preparation &amp; transfer"/><category term="pulse-level-compilation" label="Pulse-level compilation"/>    <summary type="text">Continuous-time Quantum Annealing (QA) is a strategy for preparing the ground state of nontrivial many-body systems. In its standard form, the dynamics is generated by a time-dependent interpolation between a simple driving Hamiltonian and the target problem Hamiltonian, usually implemented through a linear schedule. This approach faces the crucial bottleneck of small spectral gaps, which may require exponentially long annealing times to ensure adiabaticity. Here, we show how to implement quantum control over the annealing schedule in a frustrated Ising ring, one of the simplest models exhibiting an exponentially small bottleneck gap. By optimizing smooth continuous-time annealing schedules with a dressed-CRAB approach, and using a digitized representation of the dynamics to efficiently evaluate gradients, we construct protocols that strongly outperform standard fixed schedules. The optimized dynamics bypasses the bottleneck through a strongly nonadiabatic mechanism, leading to efficient ground-state preparation despite the exponentially small minimum gap. In particular, the annealing time required to reach a fixed residual-energy threshold is found to grow linearly with system size rather than exponentially. We further examine a lowest-order variational counter-diabatic correction and find that, once schedule optimization is allowed, it does not lead to any improvement.</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>QML-PipeGuard: Drift-Aware Behavioral Fingerprinting for Quantum Machine Learning Pipeline Integrity</title>
    <id>https://arxiv.org/abs/2605.25066</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2605.25066"/>
    <published>2026-05-24T00:00:00Z</published>
    <updated>2026-05-24T00:00:00Z</updated>
<author><name>Esra Yeniaras</name></author><category term="machine-learning-control" label="Reinforcement &amp; machine learning for control"/><category term="pulse-level-compilation" label="Pulse-level compilation"/>    <summary type="text">Quantum machine learning (QML) is moving from research prototypes to deployed cloud services. As QML enters regulated industries, the integrity of the quantum stage becomes a practical concern on two fronts: noisy hardware drifts at the channel level between recalibrations, and an adversary with control over the execution environment can substitute the declared quantum channel with a behaviorally similar but mathematically distinct one. Neither concern is covered by existing QML verification work on pulse-level noise, input drift, input-perturbation robustness, or device identity. We introduce QML-PipeGuard, a contract-based framework addressing both concerns under a single mathematical machinery. It characterizes a QML pipeline at runtime by its behavioral fingerprint, the vector of observable expectation values under a tomographically structured measurement family, and operates in two modes: drift-aware monitoring that absorbs benign calibration changes within a calibrated tolerance, and adversarial detection that catches channel substitution as a violation of an informationally complete observable contract. The framework contributes a pipeline-composition treatment of the encoder-ansatz-measurement channel with a QML-specific threat model (tight frame-bound C=sqrt(3) for the single-qubit Pauli family), a finite-shot sample-complexity bound, and a tolerance decomposition separating adversarial and natural-drift contributions. We validate the framework end-to-end on a two-qubit QSVM pipeline on the IBM Heron r2 processor (ibm_fez), with a sample-complexity validation on a noise-matched simulator. The prescribed measurement budget (about 1.4e4 shots) fits in a single batched job, the sneaky channel is detected with a wide safety margin while evading the weak contract, and the typical hardware drift sits within tolerance.</summary>
  </entry>
  <entry>
    <title>QuCtrl-BELL: A Compiler-Driven Sub-Microsecond Feedback Control Stack for Scalable Trapped-Ion Quantum Experiments</title>
    <id>https://arxiv.org/abs/2605.22433</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2605.22433"/>
    <published>2026-05-21T00:00:00Z</published>
    <updated>2026-05-21T00:00:00Z</updated>
<author><name>Junpeng She</name></author><author><name>Ruoyu Yan</name></author><author><name>Zhizhen Qin</name></author><author><name>Zhanyu Li</name></author><author><name>Zhongtao Shen</name></author><author><name>Zichao Zhou</name></author><author><name>Bin-Xiang Qi</name></author><author><name>Luming Duan</name></author><category term="feedback-control" label="Measurement-based feedback"/><category term="trapped-ions" label="Trapped ions"/><category term="control-hardware" label="Control electronics &amp; software stacks"/><category term="pulse-level-compilation" label="Pulse-level compilation"/>    <summary type="text">As trapped-ion quantum computing scales to larger qubit registers and more complex control protocols, classical control systems face a fundamental tradeoff: sub-microsecond board-level feedback requires tight hardware coupling, whereas maintainability and extensibility require clean, modular software abstractions. This paper presents QuCtrl-BELL (Bell), a compiler-driven software stack for trapped-ion quantum control. The design resolves this tradeoff by decoupling control flow -- including loops, branches, and synchronization -- from hardware state data. A Python-embedded domain-specific language (DSL) is lowered through a six-stage transpilation pipeline covering control flow graph (CFG) construction, static single-assignment (SSA) conversion, liveness analysis, and graph-coloring register allocation. The compiler generates deterministic distributed board-level programs and compact step-table data. A cross-board synchronization protocol supports feedback loops with latency below 700~ns without host intervention. Bell is deployed and evaluated on the QuCtrl-BELL platform (RISC-V + PXIe), demonstrating that a compiler-based infrastructure can provide programmability, deterministic timing, and modularity for scalable trapped-ion quantum control.</summary>
  </entry>
  <entry>
    <title>Software Between Quantum and Machine Learning -- And Down to Pulses</title>
    <id>https://arxiv.org/abs/2605.21286</id>
    <link rel="alternate" type="text/html" href="https://arxiv.org/abs/2605.21286"/>
    <published>2026-05-20T00:00:00Z</published>
    <updated>2026-06-01T00:00:00Z</updated>
<author><name>Maja Franz</name></author><author><name>Melvin Strobl</name></author><author><name>Jonathan Hunz</name></author><author><name>Lukas Scheller</name></author><author><name>Lucas van der Horst</name></author><author><name>Eileen Kuehn</name></author><author><name>Achim Streit</name></author><author><name>Wolfgang Mauerer</name></author><category term="pulse-level-compilation" label="Pulse-level compilation"/><category term="machine-learning-control" label="Reinforcement &amp; machine learning for control"/>    <summary type="text">Contemporary quantum computing platforms remain, in essence, programmable physical systems whose control is typically mediated through unitary gate abstractions. While such abstractions provide a uniform interface, they obscure important aspects of the underlying hardware and may limit the exploitation of its full capabilities. Direct operation at the control-pulse level offers a more expressive and physically faithful paradigm, enabling, for instance, the implementation of tailored error-mitigation and optimisation strategies. However, this increased expressivity comes at the cost of greater quantum software development complexity, necessitating structured and accessible tooling. We present a software framework, integrated within the QML-Essentials package, that extends quantum machine learning (QML) methodologies to encompass pulse-level modelling. By embedding quantum optimal control techniques within a QML setting, our approach enables the seamless combination of gate-based and pulse-level representations. The framework provides a comprehensive suite of modelling and analytical capabilities. In particular, we introduce composable ansatz constructions based on interchangeable building blocks, and support for end-to-end optimisation of pulse parameters. Motivated by the central role of quantum Fourier models, we further incorporate a range of Fourier-analytic diagnostics, complemented by extended measures of entanglement. All performance-critical components are implemented in a high-performance environment using JAX and supported by a dedicated quantum simulator. Taken together, the framework facilitates reproducible and systematic investigations, while bridging the conceptual and practical divide between abstract circuit models and hardware-aware optimisation. It provides a robust foundation for future developments at the intersection of QML and quantum control.</summary>
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