Papers for

quantum algorithm developers

Papers whose findings have a practical use for this group, as judged from the abstract. Open a paper to read what it means in practice.

QMA quantum proofs can always be made perfectly complete

QMA has perfect completeness

Abstract: We prove $\mathsf{QMA} = \mathsf{QMA_1}$, i.e., every quantum Merlin-Arthur proof system can be made perfectly complete. Our construction uses only Hadamard, Toffoli, and $X$ gates, yielding a universal gate set for $\mathsf{QMA_1}$. As a consequence, quantum $3$-SAT is $\mathsf{QMA}$-complete. The construction relativizes to classical oracles, so known classical-oracle separations of $\mathsf{QMA}$ from $\mathsf{QCMA}$ extend to $\mathsf{QMA_1}$.

Fri 11 SeptComputational Complexity
The gist
Some computer problems can be checked using quantum proofs, but these checks sometimes have a small chance of rejecting a correct proof. The authors show that it is possible to design these quantum proof systems so that if the proof is correct, it will always be accepted. They achieve this using a specific set of basic quantum operations. This result also confirms that an important quantum logic problem remains one of the hardest in quantum computation.
Open 2609.13032v1

Sharp continuity bounds link quantum entropy and entanglement measures

Log-Sobolev inequality, von Neumann entropy and Entanglement of Formation

Abstract: We present two results derived from the sharp log-Sobolev inequality for the uniform measure on a complete graph which concern the von Neumann entropy and the Entanglement of Formation of a state of finite and infinite-dimensional quantum systems. The first result is a sharp Lipschitz lower semicontinuity bound for the von Neumann entropy at any mixed state $ρ$ with uniform positive spectrum (i.e. a state proportional to a projector) w.r.t. the fidelity deficit: the inequality $\,S(ρ)-S(σ)\leq C_ρ(1-F(ρ,σ))\,$ valid for any state $σ$, where $C_ρ$ is a constant depending on the rank of $ρ$. The second result is a sharp Lipschitz lower semicontinuity bound for the Entanglement of Formation at any pure state $ρ$ with uniform positive spectrum of marginal states: the inequality $\,E_F(ρ)-E_F(σ)\leq \frac{1}{2}\,C_ρ\|ρ-σ\|_1\,$ valid for any state $σ$, where $C_ρ$ is a constant depending on the Schmidt rank of $ρ$. In both cases the optimal constant $C_ρ$ is equal to the optimal constant $K_{d}$ in the log-Sobolev inequality for the complete graph with $d$ vertices: in the first case $d=\mathrm{rank}ρ$, in the second one $d=\mathrm{rank}ρ_A=\mathrm{rank}ρ_B$. The authors are grateful to GPT 5.6 for valuable discussion and technical help in preparing this note.

Fri 11 SeptInformation Theory
The gist
This paper provides new mathematical bounds that tell us how much certain quantum properties, like entropy and entanglement, can change when a quantum state changes a little bit. The authors use a known inequality from graph theory to find exact constants that govern these changes. This helps to understand and measure quantum information reliably, even for complex quantum systems with many parts. These bounds work for both simple and very large quantum systems.
Open 2609.12667v1

Efficient method to learn sparse quantum states with optimal samples

Learning Sparse Quantum States

Abstract: We study the problem of tomography for $k$-sparse quantum states. In contrast to classical distribution learning, where tight sample and time complexity bounds in terms of support size are well understood, no non-trivial bounds were previously shown for this problem. We give the first near optimal algorithm for learning $n$-qubit $k$-sparse pure quantum states, obtaining fidelity at least $1-\varepsilon$ with high probability using $\tilde{O}(k/\varepsilon)$ copies of the state and $\tilde{O}(kn/\varepsilon)$ time. Both bounds are optimal up to polylogarithmic factors. As an implication, we also obtain an algorithm with near optimal $\tilde{O}(kr/\varepsilon)$ sample complexity for learning $k$-sparse rank-$r$ mixed states, via the random purification channel technique. Obtaining time complexity nearly matching the sample complexity, for $r>1$, remains an important open question.

Thu 10 SeptComputational ComplexityData Structures and Algorithms
The gist
Learning the details of complex quantum states is important but very challenging, especially when those states are mostly simple with only a few nonzero parts. The authors developed the first nearly optimal method to figure out these states using a number of samples that grows roughly with how many nonzero parts the state has. Their method also runs quickly compared to previous approaches. This work helps make it easier to understand certain quantum systems and could guide future quantum technology development.
Open 2609.12219v1

Quantum proof systems with pure states collapse into single QMA class

PureSuperQMA(exp) = BellPureSymQMA(poly) = QMA via Dimension-Free Bosonic Argmax

Abstract: Pure-state consistency problems naturally lead to quantum proof systems in which a single pure witness must satisfy many acceptance constraints. The corresponding class $\mathsf{PureSuperQMA}$ was previously known to lie between $\mathsf{QMA}$ and $\mathsf{QMA}(2)$, and Kamminga and Rudolph (ITCS'26) conjectured that both containments are strict. In this paper, we prove the following surprising complexity collapses $$ \mathsf{QMA} = \mathsf{PureSuperQMA} = \mathsf{PureSuperQMA}(\text{exp}) = \mathsf{BellPureSymQMA}(\text{poly}) $$ Here $\mathsf{PureSuperQMA}(\text{exp})$ allows exponentially many checks which are uniformly indexed and efficiently generated, while requiring an inverse-polynomial violation margin and an inverse-polynomial fraction of violated checks for the NO cases. $\mathsf{BellPureSymQMA}(\text{poly})$ is a related model that requires the prover to give the verifier polynomially many copies of a pure state, which the verifier measures separately with logarithmic output length for each local measurement, before processing the outcomes jointly. The main technical ingredient is a dimension-free stability bound for symmetric tensor states. Our simulations use polynomially many witness registers and combine a random-pair SWAP test with a permutation-invariant lift of the original verification procedure. The key step is to show that, on the symmetric subspace, the extremal verification value is close to that of some tensor-power witness with dimension-independent error. Applying this argument to the two verification models yields both simulations. As a consequence, exact $k$-local pure-state consistency is $\mathsf{QMA}$-complete for every fixed $k\ge2$, and so are the corresponding exact bosonic and fermionic pure $N$-representability problems.

Thu 10 SeptComputational Complexity
The gist
Deciding if a single pure quantum state can satisfy many constraints is a challenging problem linked to quantum complexity classes. The authors show that several previously different quantum proof classes, including one with exponentially many checks and another requiring many copies of a pure state, are all actually equivalent to the standard class QMA. This means that verifying pure quantum states is not harder than well-known quantum verification problems. Their proof uses new mathematical bounds on symmetric quantum states that do not depend on system dimension.
Open 2609.11854v1

Quantum circuit search improves with synthetic replay model

Generative Replay Mitigates Sample Starvation in Quantum Architecture Search

Abstract: Reinforcement learning (RL) can automate quantum architecture search, but its scalability is limited when useful circuit trajectories become rare in the rapidly expanding search space. Existing replay mechanisms reuse observed transitions; the proposed learned model produces additional predicted one step transitions from real state-action seeds. Here we introduce GenQAS, a tensor network-guided RL framework that combines a fixed matrix product state warm-start with prioritized generative replay. A learned local transition model generates synthetic circuit transitions on demand and mixes them with real experience during Double Deep Q-Network updates. Under a random exploration analysis, near ground state circuits occupy a rapidly shrinking region of the accessible state space. We investigate whether real data anchored synthetic replay can improve the effective training signal in this regime. Across chemical Hamiltonian benchmarks from 6 to 12 qubits, GenQAS improves fixed-budget success probability and identifies compact circuits at competitive energy error. At 12 qubits, it improves final success probability by up to $7.0\times$ over passive replay. On a 15-qubit transverse field Ising model, GenQAS increases success probability from $12\%$ to $21\%$. In a noisy 6-qubit BeH$_2$ transfer experiment, generative replay reduces the steps to chemical accuracy by $92.7\%$. These results show that generative replay can mitigate sample starvation in quantum architecture search and support more resource efficient circuit discovery.

Thu 10 SeptArtificial IntelligenceEmerging TechnologiesMachine Learning
The gist
Finding useful designs for quantum circuits can be very hard because the search space is huge and good solutions are rare. The authors introduce GenQAS, a method that teaches a computer to imagine new possible steps in building quantum circuits based on real examples it has seen. By mixing these imagined steps with real experiences, the learning process becomes more efficient. Testing this approach on chemical and physics problems showed it finds better circuits faster and more reliably. This helps make quantum circuit design more practical and resource efficient.
Open 2609.11248v1

Quantum algorithm limits revealed for hypergraph max cut problems

The Quantum Overlap Gap Property and Algorithmic Hardness for the Quantum Hypergraph Max-Cut Problem

Abstract: In this work, we analyze the average-case hardness of approximation for the Quantum Hypergraph Max-Cut problem using the theoretical framework of the Quantum Overlap Gap Property (QOGP). We establish two main results. Our first result applies to a wide class of stable quantum algorithms, satisfying a Lipschitz property with respect to the quantum Wasserstein distance of order $2$. We show a weak hardness result, demonstrating that for any Lipschitz constant $L$, there is some $k$ such that $L$-stable algorithms cannot approximate the optimal solution to Quantum Hypergraph Max-Cut on $k$-uniform hypergraphs in the average case. Additionally, we establish a strong hardness result where $k$ is independent of $L$, but only for a more restricted class of local quantum algorithms defined using the quantum Wasserstein distance of order $\infty$. We apply these results to establish concrete depth lower bounds for popular quantum algorithms for preparing near-optimal states for this problem.

Wed 9 SeptComputational Complexity
The gist
Solving the Quantum Hypergraph Max-Cut problem means finding the best way to break a complex quantum system into parts. The authors studied why some popular quantum algorithms struggle to get close to the best solution, showing there are inherent limits depending on the algorithm’s properties. They used a mathematical tool called the Quantum Overlap Gap Property to prove that for many algorithms, especially those that are stable or local, it’s impossible to approximate the best answer well. This helps explain why some quantum methods can't easily solve these problems even on average.
Open 2609.10838v1

Quantum speedup limits depend on input methods and output requirements

When Does a Quantum Speedup Survive End-to-End?

Abstract: Primitive quantum speedups are interface-relative: they depend on the input access used to run the primitive and on the output contract used to consume its state or samples. This paper introduces a transcript-level admissibility relation \(A_M\preceq_{\mathrm{int}}A_Q\), defined relative to the declared implementation package of the quantum interface. It identifies which adaptive classical access transcripts that same package licenses, with all setup, transcript-generation, and precision overheads charged. The main application is an operational audit for normalized-Betti estimation in clique-complex TDA, separating three declared-interface regimes. Reversible indexed simplex interfaces certify matched classical simplex sampling and local Laplacian row access by evaluating their reversible routines on single computational branches. Membership-based preparations induce a rejection route of overhead \(\binom{n}{k+1}/|S_k|\). Abstract spectral or block-encoding interfaces require an accompanying implementation package, transcript reduction, or shared representation. Under the indexed certificate and interface closure, the end-to-end cost is fixed by the imported estimator's spectral dependence on the gap \(γ\); the concretely realized bounded-treewidth family already admits exact \(\mathrm{poly}(n)\) classical Betti computation by rank over \(\mathbb{Q}\). A low-rank separation supports the role of access and output contracts.

Wed 9 SeptComputational Complexity
The gist
Quantum computers can sometimes solve problems faster than classical ones, but whether this speed advantage holds true depends on exactly how you feed data in and get answers out. The authors study how different ways of accessing and using a quantum routine affect its overall cost and speed, using a detailed model of interactions. They focus on a complex math problem called Betti number estimation, showing that some quantum speedups may disappear when considering the entire process, while others can survive with the right interfaces. Their work helps clarify when quantum speedups are meaningful from start to finish.
Open 2609.09850v1

Quantum algorithms cannot quickly 4-color directed cycles accurately

Impossibility of One-Way One-Round Quantum 4-Coloring via Matrix-Space Stability

Abstract: We show that one-way one-round quantum LOCAL algorithms cannot $4$-color directed cycles with high probability, even with unbounded local computation and quantum message length. This is the first lower bound in the high-probability quantum LOCAL setting that goes beyond the non-signaling and bounded-dependence models, exploiting the structure of distributed quantum algorithms. Our proof connects distributed quantum computing with noncommutative extremal combinatorics by identifying local collision probabilities with the weighted multiplicative energy of matrix-space decompositions. We obtain our lower bound by proving a dimension-independent weighted stability theorem for a directed noncommutative analogue of Mantel's theorem.

Tue 8 SeptDistributed, Parallel, and Cluster Computing
The gist
This paper shows that certain fast quantum algorithms cannot reliably solve the problem of coloring directed cycle graphs with four colors without conflicts. The authors prove this even if the algorithm can perform unlimited local computation and send very long quantum messages, emphasizing inherent limits of distributed quantum computing. Their approach connects the problem to advanced mathematics involving matrix spaces and combinatorics, revealing deep structural reasons why the problem is hard. This is the first such high-probability lower bound in this quantum setting, going beyond previous simpler models.
Open 2609.09091v1

QAOA performance improved by error detection for better optimization results

Toward Fault-Tolerant Variational Optimization: QAOA under [[4,2,2]] Error Detection

Abstract: We present a partially fault-tolerant implementation of QAOA based on the $[[4,2,2]]$ error-detection code, targeting the Max-Cut problem on a square graph. Our main contribution is a novel ancilla-mediated logical $R_{ZZ}$ gate enabling interactions between qubits in different $[[4,2,2]]$ blocks. We evaluate unencoded and encoded circuits under five noise models, with both all-to-all and grid-routed connectivity, using the Cirq and qsimcirq frameworks with parallel CPU execution. Post-selection on stabilizer measurements consistently improves the probability of sampling optimal bitstrings, with five measurements providing the strongest benefit. These results support error-detection as a practical near-term strategy for improving the quality of variational quantum algorithms.

Mon 7 SeptEmerging Technologies
The gist
Quantum computers need to handle errors to work well. This paper shows how using a special error-detecting code can improve a quantum algorithm called QAOA, which tries to solve optimization problems. The authors designed a new way for parts of the computer to talk while checking for errors. Their tests suggest this error-detection method can help get better answers more often, making quantum optimization more reliable in the near future.
Open 2609.07537v1

Asymmetric quantum error correction improves noise handling in quantum algorithms

Asymmetric quantum error correction efficiently tackles application-specific noise effects

Abstract: Noise is a major challenge for current quantum computers. It can be broadly categorized into bit-flip and phase-flip errors. These two types do not necessarily affect the executed algorithm, thus also the application, in the same way. We illustrate this general effect for the example of the quantum approximate optimization algorithm (QAOA) applied to a small instance of the flight-gate assignment (FGA) problem. We compare bit-flip and phase-flip Pauli noise under both layer-level and gate-level noise models, using two circuit decompositions of the same ideal QAOA unitary: a CNOT-based decomposition and a native-$R_{ZZ}$ decomposition. In the simulations, bit-flip noise produces the larger degradation in the performance of the quantum optimization. The asymmetry is most visible in the layer-level and native-$R_{ZZ}$ simulations. We explain this by how the errors affect mixing, final measurements, and how they propagate inside the circuit. We then exploit these insights to tackle noise particularly efficiently using asymmetric error-correcting codes. As an illustration, we use the quantum parity code (QPC), a generalization of the 9-qubit Shor code, and show that a smaller asymmetric code can achieve nearly the same improvement as a larger symmetric choice. This demonstrates that error-correction resources should be assigned not only according to physical error rates, but also according to how strongly each error channel affects the application. As a result, asymmetric quantum error correction proves useful even in cases where the noise model is symmetric. Finally, we discuss how information about the noise obtained through calibration can be exploited in our approach.

Mon 7 SeptEmerging Technologies
The gist
Quantum computers face errors that can flip bits or change phases, and these errors affect tasks differently. The authors studied a quantum optimization algorithm and found that bit-flip errors hurt its performance more than phase-flip errors. They showed that using error-correcting codes tailored to these differences can protect computations more efficiently. This approach even helps when the overall noise is balanced, by focusing resources on the more damaging error type.
Open 2609.07235v1