REVIEW 3 major objections 6 minor 8 cited by
A Framework for Quantum Advantage
T0 review · 3 major / 6 minor · reviewed 2026-08-06 · deepseek-v4-flash
Pith's one-line read The paper argues that quantum advantage requires both rigorous validation of outputs and a demonstrable separation from classical computation, and that random circuit sampling does not yet meet this bar.
desk verdict A coherent, useful position paper on quantum advantage whose dismissal of RCS depends on a validation standard applied unevenly; worth engaging, but the asymmetry needs confrontation. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The load-bearing object is a two-criterion definition of quantum advantage, coupled with a taxonomy of validation modes. Validation, the first criterion, can be achieved in three ways: rigorous error bars (from fault-tolerant computation, formally proven error mitigation, or post-selected error detection); efficient classical verification of the answer's structure (as in factoring or peaked sampling); or variational scoring, where approximate solutions can be ranked by energy or cost without knowing the exact answer. The second criterion, quantum separation, requires the quantum result to be demonstrably better than the best available classical approach, measured by efficiency, cost, or accuracy. This definitional machinery does the work of classifying algorithms: it elevates sample-based quantum diagonalization and error-mitigated expectation values as verifiable, and demotes random circuit sampling as unverifiable at scale.
What would settle it
A random-circuit-sampling experiment whose outputs are certified by a method the community accepts as rigorous—for example, fault-tolerant or post-selected error-detected sampling—and whose distribution is verified classically at a scale beyond classical simulation would falsify the claim that RCS is not a satisfactory pathway to quantum advantage.
Extended reading notes
Core claim
On the paper's own terms, the central discovery is a definition plus a verdict. Quantum advantage is defined as the execution of an information-processing task on quantum hardware that satisfies two criteria: (i) the correctness of the output can be rigorously validated, and (ii) the computation is performed with a quantum separation that demonstrably offers superior efficiency, cost-effectiveness, or accuracy over classical computation alone. The paper then applies this definition to three algorithmic families—sampling, variational ground-state problems, and expectation values of observables—and concludes that random circuit sampling does not yet constitute a fully satisfactory pathway to quantum advantage, because the only universally accepted way to certify that RCS outputs are drawn faithfully at scale is fault-tolerant quantum computing. Experimental supremacy claims based on RCS therefore remain unsubstantiated under this criterion. In contrast, sample-based quantum diagonalization and error-mitigated expectation values with provable error bounds achieve the highest degree of verifiability, because their outputs can be classically ranked and reproduced, making them the most credible candidates for early advantage.
Load-bearing premise
The paper's verdict depends on the normative judgment that statistical certification of sampling outputs is not validation; if the community instead accepts cross-entropy benchmarking or similar statistical evidence as sufficient, the conclusion that RCS claims are unsubstantiated collapses.
Editorial extensions
If this is right
- Random-circuit-sampling claims will not count as quantum advantage under this standard until sampling is certified by fault tolerance, error detection with post-selection, or an equally rigorous method.
- Early advantage claims will most plausibly come from classically verifiable ground-state problems, such as sample-based quantum diagonalization, where the final answer is stored and checked classically.
- Error mitigation with proven error bounds, augmented by classical tensor-network and light-cone methods, extends the reach of expectation-value computations beyond brute-force classical simulation.
- The benchmark for advantage shifts from quantum-hardware-versus-classical to hybrid quantum-classical systems integrated into HPC, so advantage becomes a property of the combined workflow.
- Peaked random circuits are the remaining open avenue for sampling-based advantage, pending a rigorous hardness analysis; quasi-polynomial classical simulation of peakedness threatens them.
Reading between the lines
- Editorial extension: the paper's definition makes community acceptance of statistical certification, such as cross-entropy benchmarking, the decisive judgment; if that judgment flips, so does the verdict on RCS.
- Editorial extension: the 'quantum separation' criterion compares against best-known classical algorithms and hardware-specific metrics, so in practice the framework yields sequential, falsifiable benchmarks rather than unconditional separations.
- Editorial extension: the constructive path depends on the paper's own caveat that error mitigation has exponential sampling overhead and analog verification is hard; if hardware fidelity plateaus, the expectation-value route weakens.
- Editorial extension: a direct testable next step is identifying which local observables in analog simulators keep size-independent error bounds, using the cited robustness results as a map.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This position paper proposes a functional definition of quantum advantage with two criteria: (i) the correctness of the output can be rigorously validated, and (ii) the computation is performed with a quantum separation that demonstrably offers superior efficiency, cost-effectiveness, or accuracy over classical computation. The authors apply this framework to three algorithmic families: sampling problems, variational/diagonalization methods, and expectation-value estimation. They conclude that random circuit sampling (RCS) does not yet constitute a satisfactory pathway to quantum advantage because its outputs cannot be rigorously validated at scale without fault tolerance, whereas error-mitigated expectation values and quantum diagonalization methods (SQD/SKQD) are more likely to yield early, verifiable advantage. The paper also reviews error correction, error mitigation, error detection, quantum-centric supercomputing, and current hardware platforms.
Significance. If accepted, the proposed definition would provide a much-needed common vocabulary for evaluating near-term quantum advantage claims, and the paper's emphasis on verifiability, falsifiability, and open benchmarking is a constructive contribution to the field. The manuscript is clearly written and well-referenced, and it gives a detailed, honest discussion of error detection as an intermediate path between error mitigation and fault tolerance. The paper's concrete roadmap—prioritizing error-mitigated expectation values and diagonalization-based methods over sampling—is a useful hypothesis that can stimulate further research. However, the paper is a perspective rather than a proof-based contribution, and its central applied conclusion about RCS rests on a normative epistemic standard that is applied asymmetrically to the methods it favors. The definition itself also lacks an operational specification of what counts as 'demonstrably superior.' These issues do not destroy the paper's value but do require substantial clarification before the conclusions can be considered fully supported.
major comments (3)
- [Section III vs. Section IV A2] The validation standard is applied unevenly. Section III rejects RCS because XEB-style statistical certification is treated as insufficient, asserting that 'the only universally accepted method for achieving this is fault-tolerant quantum computing.' Yet Section IV A2 claims that several quantum error mitigation methods 'have demonstrated the ability to yield accurate expectation values from short-depth circuits, with rigorous error bounds [60,61].' Those rigorous error bounds are conditional on noise-model assumptions (e.g., sparse Pauli-Lindblad models) that are themselves verified only through heuristic evidence such as randomized benchmarking and small-system tomography. Section II A concedes that 'formally proven results always rely on a set of initial assumptions... that must themselves be verified.' At scales beyond classical simulation, those noise-model assumptions cannot be fully verified independently, leaving a symmetric vulnerability to unmodeled errors. The paper does not supply a principled boundary between heuristic validation that is admissible and heuristic validation that is not; this asymmetry is load-bearing because it drives the central conclusion that RCS is not a satisfactory pathway while error-mitigated expectation values are.
- [Section III, RCS paragraph] The assertion that fault-tolerant quantum computing is the 'only universally accepted method' for certifying error-free sampling is a contestable empirical claim about community consensus, not a technical result. The paper does not engage with the substantial literature on verification of random circuit sampling, including linear cross-entropy benchmarking and its known limitations, nor does it explain why statistical evidence of sampling correctness is categorically inadmissible while the statistical evidence supporting noise-model accuracy is admissible. Because the RCS conclusion depends entirely on this premise, the authors should either justify the consensus claim with evidence or reframe it explicitly as a normative choice rather than a universal standard.
- [Section II, Definition of quantum advantage] The second criterion—'quantum separation that demonstrably offers superior efficiency, cost-effectiveness, or accuracy'—is not operational as stated. The paper does not specify the baseline (e.g., best known classical algorithm at the time of the claim, including future algorithmic improvements), the metric (wall-clock time, financial cost, energy, accuracy measure), or the required confidence level. The abstract calls the definition 'empirically verifiable,' but without these specifications it is difficult to falsify any particular claim of advantage. This weakens the central contribution of the paper, which purports to provide a functional framework for evaluating advantage claims.
minor comments (6)
- [Section I] The paper uses 'quantum advantage' without clarifying its relationship to the earlier term 'quantum supremacy'; a sentence distinguishing the two would help readers.
- [Section III, peaked random circuits] The paragraph on peaked random circuits first presents peakedness as enabling verifiable advantage and then notes that peaked distributions may be simulable in quasi-polynomial time [29]; the presentation would be clearer if this tension were addressed head-on rather than leaving the reader to reconcile the two statements.
- [Section IV A2] The PEC sampling overhead expression '~ (1+15ε/8)^{nd}' should define n, d, and ε explicitly and state the noise model to which ε refers.
- [Section IV B] The term 'quantum-centric supercomputing (QCSC)' is used as a proprietary label; consider defining it in more neutral language so the framework is accessible to a broad community.
- [Section V] The prediction that credible evidence of quantum advantage will emerge 'within the next two years' is speculative and lacks supporting analysis; either cite a roadmap study or soften the claim.
- [Throughout] Several statements are phrased as opinions ('we believe,' 'we anticipate') mixed with technical assertions; marking the distinction would improve clarity in a position paper.
Circularity Check
No significant circularity: the paper's conclusions follow from its stipulated definition of quantum advantage, and the cited supporting results are published, independently checkable works rather than inputs fitted here.
full rationale
The paper stipulates in Section II that quantum advantage requires rigorous validation and a demonstrable quantum separation. The later conclusion about random circuit sampling, 'we conclude that random circuit sampling (RCS) does not yet constitute a fully satisfactory pathway to quantum advantage,' is a classification under that stipulated criterion, not an empirical prediction derived from the definition by a hidden fit. No parameter is fitted to data and then renamed as a prediction; no uniqueness theorem from the authors' prior work is invoked to force the choice of methods. The cited error-mitigation bounds and sample-based quantum diagonalization results (e.g., refs. [60, 61, 9]) are real published results with stated assumptions, even though some authors overlap with the present paper. The perceived asymmetry between statistical certification for RCS and noise-model-based certification for error mitigation is a normative epistemic judgment about what counts as validation; it may be debated as a correctness or fairness concern, but it is not a derivation loop. The framework is self-contained relative to its own definitions, and the applied conclusions are conditional on those definitions rather than equivalent to them by construction.
Assumptions & free parameters
assumptions (4)
- domain assumption The correctness of a quantum computation must be established through rigorous error bars or efficient classical verification of the output.
- domain assumption Fault-tolerant quantum computing is the only universally accepted method to certify random circuit sampling outputs at scale.
- standard math The variational principle permits classical ranking of approximate ground-state energies.
- domain assumption The relevant comparison for quantum advantage is the hybrid quantum-classical system, not the quantum processor in isolation.
Cite this review
Pith. "Pith review of A Framework for Quantum Advantage." pith.science (2026). https://pith.science/paper/BMYZSKMD
@misc{pith2026250620658,
author = {Pith},
title = {Pith review of: A Framework for Quantum Advantage},
year = {2026},
howpublished = {\url{https://pith.science/paper/BMYZSKMD}},
note = {Machine review of arXiv:2506.20658}
}
read the original abstract
As quantum computing approaches the threshold where certain tasks demonstrably outpace their classical machines, the need for a precise, clear, consensus-driven definition of quantum advantage becomes essential. Rapid progress in the field has blurred this term across companies, architectures, and application domains. Here, we aim to articulate an operational definition for quantum advantage that is both platform-agnostic and empirically verifiable. Building on this framework, we highlight the algorithmic families most likely to achieve early advantage. Finally, we outline our vision for the near future, in which quantum computers enhance existing high-performance computing platforms, enabling new frontiers in chemistry, materials discovery, optimization, and beyond.
Forward citations
Cited by 8 Pith papers
-
Sampling hard circuits with verifiably high fidelity
A 97-qubit experiment certifies a 0.284 fidelity lower bound for a 468-T-gate sampling circuit by combining spacetime-code error detection with the measured fidelity of an undoped Clifford reference.
-
Logarithmic growth of operator entanglement in a clean non-integrable circuit
In a clean non-integrable semi-ergodic dual-unitary circuit, operator entanglement of a local Pauli grows at most logarithmically in time, with bimodal operator-size distributions and late-time autocorrelations matchi...
-
Syndrome aware mitigation of logical errors
Conditioning logical error mitigation on the measured error-correcting syndromes cuts sampling overhead exponentially and can make error correction useful above its standard pseudo-threshold.
-
Universal initial state preparation for first quantized quantum simulations
By mapping Fock occupations to Schur labels via the Jordan-Schwinger homomorphism and applying an inverse quantum Schur transform, the paper constructs a first-quantized state-preparation protocol with poly(L,N,log d,...
-
Systematic Experiment Tracking in Quantum Software: A Case Study of Reservoir Computing with Error Mitigation
MLflow-style experiment tracking, extended with quantum provenance, supports reproducible multi-stage quantum software pipelines, shown on error-mitigated quantum reservoir computing for chaotic time-series prediction.
-
Observation of Robust and Coherent Non-Abelian Hadron Dynamics on Noisy Quantum Processors
A 60-site SU(2) lattice gauge theory was run on 120 qubits, but the implemented dynamics approximate to non-interacting fermion hopping, and the abstract's claimed breathing-mode frequency is not extracted anywhere.
-
Dissipative ground-state preparation of a quantum spin chain on a trapped-ion quantum computer
A trapped-ion experiment prepared low-energy states of a 19-spin Ising chain by engineered dissipation, backed by an exact finite-step Kraus form of the cooling channel.
-
The vast world of quantum advantage
Assuming quantum computers are strictly more powerful than classical ones, the problem of deciding whether a given quantum circuit beats a specific classical simulation heuristic is solvable by quantum computers but n...
Reference graph
Works this paper leans on
-
[1]
The way to achieve this formally is through proven error bars
Error bars and error bounds A universal way to ensure that the computation can be trusted is to ensure that every step of the computation was performed accurately. The way to achieve this formally is through proven error bars. There are different methods that can ensure such error bars, the car- dinal approach being fault-tolerant quantum computing, cf. S...
arXiv 2025
-
[2]
But some of these problems are structured in such a way that, once found, these answers can be verified efficiently on a classical computer
Problems with efficient classical verificationIt is believed that for certain problems the answers can only be found effi- ciently on a quantum computer. But some of these problems are structured in such a way that, once found, these answers can be verified efficiently on a classical computer. Examples include sampling problems, cf. Section III, where we ...
-
[3]
peaked- ness
Variational problems Similarly, there are problems for which it may not be possible to efficiently verify the solution on a classical computer directly, but we can easily score the quality of a solution and compare it with competing classical approaches. This is, for example, the case in variational prob- lems, cf. Section III, such as in the estimation o...
-
[4]
Error correction Quantum error correction [50] (QEC) refers to a set of techniques designed to protect quantum infor- mation from decoherence, gate imperfections, and measure- ment errors—limitations intrinsic to any practical quantum computing platform. In QEC, information is encoded into log- ical qubits: fault-tolerant constructs built from multiple ph...
-
[5]
Error mitigationQuantum error mitigation (QEM) encom- passes a suite of techniques aimed at reducing—or in some cases, eliminating—the bias in expectation value estimates caused by noise in quantum circuits [42, 56]. Unlike quan- tum error correction (QEC), QEM operates through classical post-processing of noisy outputs from ensembles of circuit ex- ecuti...
-
[6]
Conceptually, one can view the distinction between error cor- rection and error mitigation as a trade-off between quantum and classical resources—qubits versus sampling
Error detection Post-selected quantum error detection methods represent a promising intermediate approach between full quantum error correction and classical error mitigation. Conceptually, one can view the distinction between error cor- rection and error mitigation as a trade-off between quantum and classical resources—qubits versus sampling. Error detec...
2026
-
[7]
R. P. Feynman, International Journal of Theoretical Physics 21, 467 (1982)
1982
-
[8]
P. W. Shor, SIAM Journal on Computing26, 1484–1509 (1997)
1997
Show all 94 references
-
[9]
Deutsch, Proceedings of the Royal Society A 400, 97–117 (1985)
D. Deutsch, Proceedings of the Royal Society A 400, 97–117 (1985)
1985
-
[10]
A. W. Harrow, A. Hassidim, and S. Lloyd, Physical Review Letters 103 (2009)
2009
-
[11]
Lloyd, Science 273, 1073–1078 (1996)
S. Lloyd, Science 273, 1073–1078 (1996)
1996
-
[12]
Grover, Physical Review Letters 79, 325–328 (1997)
L. Grover, Physical Review Letters 79, 325–328 (1997)
1997
-
[13]
Preskill, Quantum 2, 79 (2018)
J. Preskill, Quantum 2, 79 (2018)
2018
-
[14]
Y. Kim, A. Eddins, S. Anand, K. X. Weia, E. van den Bergand Sami Rosenblatt, et al., Nature 618, 500 (2023)
2023
-
[15]
Robledo-Moreno, M
J. Robledo-Moreno, M. Motta, H. Haas, A. Javadi-Abhari, P. Ju- rcevic, et al., Science Advances 11, eadu9991 (2025)
2025
- [16]
-
[17]
D. Wu, R. Rossi, F. Vicentini, N. Astrakhantsev, F. Becca,et al., Science 386, 296 (2024)
2024
-
[18]
D. A. Abanin, R. Acharya, L. Aghababaie-Beni, G. Aigeldinger, A. Ajoy, et al., arXiv preprint arXiv:2506.10191 (2025)
2025 arXiv
-
[19]
Filippov, M
S. Filippov, M. Leahy, M. A. C. Rossi, and G. Garc ´ıa-P´erez, (2023), arXiv:2307.11740 [quant-ph]
2023 arXiv
-
[20]
Haghshenas, E
R. Haghshenas, E. Chertkov, M. Mills, W. Kadow, S.-H. Lin, et al., (2025), arXiv:2503.20870
2025 arXiv
-
[21]
Bravyi, D
S. Bravyi, D. Gosset, and R. K ¨onig, Science 362, 308 (2018)
2018
- [22]
- [23]
-
[24]
T. Koch, D. E. B. Neira, Y. Chen, G. Cortiana, D. J. Egger,et al., (2025), arXiv:2504.03832
2025 arXiv
-
[25]
Cazals, A
P. Cazals, A. Franc ¸ois, L. Henriet, L. Leclerc, M. Marin,et al., (2025), arXiv:2502.04291
2025 arXiv
-
[26]
Brodoloni, J
L. Brodoloni, J. Vovrosh, S. Juli`a-Farr´e, A. Dauphin, and S. Pi- lati, arXiv preprint arXiv:2505.05117 (2025). 8
2025
-
[27]
Arute, K
F. Arute, K. Arya, R. Babbush, D. Bacon, J. C. Bardin, et al., Nature 574, 505 (2019)
2019
-
[28]
Villalonga, X
B. Villalonga, X. Mi, S. Mandra, A. Bengtsson, P. Klimov,et al., Nature 634, 328 (2024)
2024
-
[29]
DeCross, R
M. DeCross, R. Haghshenas, M. Liu, E. Rinaldi, J. Gray, et al., Phys. Rev. X15, 021052 (2025)
2025
-
[30]
Fujii, arXiv preprint arXiv:1610.03632 (2016)
K. Fujii, arXiv preprint arXiv:1610.03632 (2016)
2016 arXiv
- [31]
-
[32]
A. L. Shaw, Z. Chen, J. Choi, D. K. Mark, P. Scholl, R. Finkel- stein, A. Elben, S. Choi, and M. Endres, Nature628, 71 (2024)
2024
-
[33]
T. I. Andersen, N. Astrakhantsev, A. H. Karamlou, J. Berndts- son, J. Motruk, et al., Nature 638, 79 (2025)
2025
-
[34]
Kechedzhi, S
K. Kechedzhi, S. V. Isakov, S. Mandr `a, B. Villalonga, X. Mi, S. Boixo, and V. Smelyanskiy, Future Generation Computer Systems 153, 431 (2024)
2024
- [35]
-
[37]
Peruzzo, J
A. Peruzzo, J. McClean, P. Shadbolt, M.-H. Yung, X.-Q. Zhou, et al., Nature communications 5, 4213 (2014)
2014
-
[38]
Kandala, A
A. Kandala, A. Mezzacapo, K. Temme, M. Takita, M. Brink, J. M. Chow, and J. M. Gambetta, Nature549, 242 (2017)
2017
-
[39]
H. R. Grimsley, S. E. Economou, E. Barnes, and N. J. Mayhall, Nature communications 10, 3007 (2019)
2019
-
[40]
Ceperley, G
D. Ceperley, G. V. Chester, and M. H. Kalos, Physical Review B 16, 3081 (1977)
1977
-
[41]
Wecker, M
D. Wecker, M. B. Hastings, and M. Troyer, Phys. Rev. A 92, 042303 (2015)
2015
-
[42]
Zhang, X
Y. Zhang, X. Zhang, J. Sun, H. Lin, Y. Huang, D. Lv, and X. Yuan, Wiley Interdisciplinary Reviews: Computational Molecular Science 15, e70020 (2025)
2025
-
[43]
Yoshioka, M
N. Yoshioka, M. Amico, W. Kirby, P. Jurcevic, A. Dutt, et al., (2024), arXiv:2407.14431
2024 arXiv
-
[44]
Kanno, M
K. Kanno, M. Kohda, R. Imai, S. Koh, K. Mitarai, W. Mizukami, and Y. O. Nakagawa, (2023), arXiv:2302.11320 [quant-ph]
2023 arXiv
-
[45]
J. Yu, J. R. Moreno, J. T. Iosue, L. Bertels, D. Claudino, et al., (2025), arXiv:2501.09702
2025
-
[46]
Kirby, Quantum 8, 1457 (2024)
W. Kirby, Quantum 8, 1457 (2024)
2024
-
[47]
Havl´ıˇcek, A
V. Havl´ıˇcek, A. D. C´orcoles, K. Temme, A. W. Harrow, A. Kan- dala, J. M. Chow, and J. M. Gambetta, Nature567, 209 (2019)
2019
-
[49]
Kandala, K
A. Kandala, K. Temme, A. D. C ´orcoles, A. Mezzacapo, J. M. Chow, and J. M. Gambetta, Nature567, 491 (2019)
2019
-
[50]
J.-y. Choi, S. Hild, J. Zeiher, P. Schauß, A. Rubio-Abadal, T. Yef- sah, V. Khemani, D. A. Huse, I. Bloch, and C. Gross, Science 352, 1547 (2016), arXiv:1604.04178 [cond-mat.quant-gas]
2016 arXiv
-
[51]
Trivedi, A
R. Trivedi, A. Franco Rubio, and J. I. Cirac, Nature Communi- cations 15, 6507 (2024)
2024
-
[52]
Y. Cai, Y. Tong, and J. Preskill, in19th Conference on the Theory of Quantum Computation, Communication and Cryptography (TQC 2024), Vol. 310 (2024) pp. 2:1–2:15
2024
-
[53]
A. J. Daley, I. Bloch, C. Kokail, S. Flannigan, N. Pearson, M. Troyer, and P. Zoller, Nature607, 667 (2022)
2022
-
[54]
R.-C. Guo, Y. Gu, and D. E. Liu, npj Quantum Information 11, 14 (2025)
2025
-
[55]
Steckmann, D
T. Steckmann, D. Luo, Y.-X. Wang, S. R. Muleady, A. Seif, C. Monroe, M. J. Gullans, A. V. Gorshkov, O. Katz, and A. Schuckert, Error mitigation of shot-to-shot fluctuations in analog quantum simulators (2025), arXiv:2506.16509
2025 arXiv
-
[56]
P. W. Shor, Phys. Rev. A52, R2493 (1995)
1995
-
[57]
A. G. Fowler, M. Mariantoni, J. M. Martinis, and A. N. Cleland, Phys. Rev. A86, 032324 (2012)
2012
-
[58]
Benito, E
C. Benito, E. L ´opez, B. Peropadre, and A. Bermudez, Quantum 9, 1623 (2025)
2025
-
[59]
Bravyi, A
S. Bravyi, A. W. Cross, J. M. Gambetta, D. Maslov, P. Rall, and T. J. Yoder, Nature627, 778 (2024)
2024
-
[60]
A. Y. Kitaev, (1995), arXiv:quant-ph/9511026 [quant-ph]
1995 arXiv
-
[61]
Clinton, T
L. Clinton, T. S. Cubitt, R. Garcia-Patron, A. Montanaro, S. Stanisic, and M. Stroeks, (2024), arXiv:2410.21517 [quant- ph]
2024 arXiv
-
[62]
Li and S
Y. Li and S. C. Benjamin, Phys. Rev. X 7, 021050 (2017)
2017
-
[63]
P. D. Nation, H. Kang, N. Sundaresan, and J. M. Gambetta, PRX Quantum 2, 040326 (2021)
2021
-
[64]
van den Berg, Z
E. van den Berg, Z. K. Minev, and K. Temme, Phys. Rev. A105, 032620 (2022)
2022
-
[65]
Giurgica-Tiron, Y
T. Giurgica-Tiron, Y. Hindy, R. LaRose, A. Mari, and W. J. Zeng, in 2020 IEEE International Conference on Quantum Computing and Engineering (QCE) (IEEE, 2020) pp. 306–316
2020
-
[66]
Temme, S
K. Temme, S. Bravyi, and J. M. Gambetta, Phys. Rev. Lett.119, 180509 (2017)
2017
-
[67]
van den Berg, Z
E. van den Berg, Z. K. Minev, A. Kandala, and K. Temme, Nature Physics 19, 1116 (2023)
2023
- [68]
-
[69]
Temme, E
K. Temme, E. van den Berg, A. Kandala, and J. Gambetta, https://www.ibm.com/quantum/blog/ gammabar-for-quantum-advantage (2022), blog post
2022
-
[70]
Aharonov, O
D. Aharonov, O. Alberton, I. Arad, Y. Atia, E. Bairey, et al., arXiv preprint arXiv:2503.17243 (2025)
2025 arXiv
-
[71]
Zimbor ´as, B
Z. Zimbor ´as, B. Koczor, Z. Holmes, E.-M. Borrelli, A. Gily´en, et al., arXiv:2501.05694 (2025)
2025 arXiv
-
[72]
L. E. Fischer, M. Leahy, A. Eddins, N. Keenan, D. Ferracin, et al., (2024), arXiv:2411.00765
2024
- [73]
-
[74]
Carrera Vazquez, D
A. Carrera Vazquez, D. J. Egger, D. Ochsner, and S. Woerner, Quantum 7, 1067 (2023)
2023
-
[75]
Harper and S
R. Harper and S. T. Flammia, Phys. Rev. Lett. 122, 080504 (2019)
2019
-
[76]
R. S. Gupta, N. Sundaresan, T. Alexander, C. J. Wood, S. T. Merkel, et al., Nature 625, 259 (2024)
2024
-
[77]
Bluvstein, S
D. Bluvstein, S. J. Evered, A. A. Geim, S. H. Li, H. Zhou,et al., Nature 626, 58 (2024)
2024
-
[78]
B. W. Reichardt, D. Aasen, R. Chao, A. Chernoguzov, W. van Dam, et al., Demonstration of quantum computation and error correction with a tesseract code (2024), arXiv:2409.04628
2024 arXiv
-
[79]
B. W. Reichardt, A. Paetznick, D. Aasen, I. Basov, J. M. Bello- Rivas, et al., Fault-tolerant quantum computation with a neutral atom processor (2025), arXiv:2411.11822
2025 arXiv
-
[80]
C. N. Self, M. Benedetti, and D. Amaro, Nature Physics20, 219 (2024)
2024
-
[81]
Tsubouchi, Y
K. Tsubouchi, Y. Mitsuhashi, R. Takagi, and N. Yoshioka, (2025), arXiv:2503.13114
2025
-
[82]
Bonet-Monroig, R
X. Bonet-Monroig, R. Sagastizabal, M. Singh, and T. E. O’Brien, Phys. Rev. A98, 062339 (2018)
2018
-
[83]
van den Berg, S
E. van den Berg, S. Bravyi, J. M. Gambetta, P. Jurcevic, D. Maslov, and K. Temme, Phys. Rev. Res.5, 033193 (2023)
2023
-
[84]
Fuller, M
B. Fuller, M. C. Tran, D. Lykov, C. Johnson, M. Rossmannek, et al., arXiv preprint arXiv:2502.01897 (2025)
2025 arXiv
-
[85]
Liepuoniute, K
I. Liepuoniute, K. D. Doney, J. R. Moreno, J. A. Job, W. S. Friend, and G. O. Jones, Journal of Chemical Theory and Com- putation 21 (2025)
2025
-
[86]
Sitdikov, M
I. Sitdikov, M. E. Sahin, U. Bacher, A. Wennersteen, A. Damin, et al., (2025), arXiv:2506.10052
2025
-
[87]
Kjaergaard, M
M. Kjaergaard, M. E. Schwartz, J. Braum¨ uller, P. Krantz, J. I.- J. Wang, S. Gustavsson, and W. D. Oliver, Annual Review of Condensed Matter Physics 11, 369 (2020)
2020
-
[88]
Saffman, T
M. Saffman, T. G. Walker, and K. Mølmer, Rev. Mod. Phys.82, 2313 (2010). 9
2010
-
[89]
C. D. Bruzewicz, J. Chiaverini, R. McConnell, and J. M. Sage, Applied physics reviews6 (2019)
2019
-
[90]
D. C. McKay, I. Hincks, E. J. Pritchett, M. Carroll, L. C. G. Govia, and S. T. Merkel, arXiV (2023)
2023
-
[91]
Acharya, D
R. Acharya, D. A. Abanin, L. Aghababaie-Beni, I. Aleiner, T. I. Andersen, et al., Nature (2024)
2024
-
[92]
Bravyi, O
S. Bravyi, O. Dial, J. M. Gambetta, D. Gil, and Z. Nazario, Journal of Applied Physics 132 (2022)
2022
-
[93]
Community, qiskit-device-benchmarking (2025), version 564164b, retrieved June 23, 2025
Q. Community, qiskit-device-benchmarking (2025), version 564164b, retrieved June 23, 2025
2025
-
[94]
Javadi-Abhari, M
A. Javadi-Abhari, M. Treinish, K. Krsulich, C. J. Wood, J. Lish- man, et al., (2024), arXiv:2405.08810
2024 arXiv
-
[95]
Henriet, L
L. Henriet, L. Beguin, A. Signoles, T. Lahaye, A. Browaeys, G.-O. Reymond, and C. Jurczak, Quantum 4, 327 (2020)
2020
-
[96]
Wurtz, A
J. Wurtz, A. Bylinskii, B. Braverman, J. Amato-Grill, S. H. Cantu, et al., (2023), arXiv:2306.11727 [quant-ph]
2023 arXiv
Reviewed August 6, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.