REVIEW 4 major objections 6 minor 63 references
Towards secondary structure prediction of longer mRNA sequences using a quantum-centric optimization scheme
T0 review · 4 major / 6 minor · reviewed 2026-08-15 · deepseek-v4-flash
Pith's one-line read The paper claims that hybrid quantum-classical optimization can find certified optimal solutions to the mRNA-folding QUBO at 156 qubits, corresponding to 60-nucleotide sequences.
desk verdict Real hardware at 156 qubits, but the Appendix A reduction is not exact, so the headline results may be for different QUBOs. 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 the QUBO in Eq. (2), whose binary variables are quartets, two consecutive base pairs written as $(i,j,i+1,j-1)$. Its energy coefficients come from empirical nearest-neighbor thermodynamics; a reward $r$ strengthens consecutive stacked quartets, a penalty $p$ discourages quartets ending in a UA pair, and a penalty $t$ forbids crossing quartets. Two mechanisms carry the variational workflow: the CVaR objective, which averages the lowest $\alpha=0.2$ tail of sampled energies and makes updates more robust to noise; and the bit-flip gauge transformation, which relabels eigenstates so that the hardware's noisy Hamming-weight bias matches the low-weight solutions expected of these dense problems. For the IQP route, the key identity is Eq. (5): expectation values of the parameterized IQP circuit reduce to a cosine sum over uniformly random bitstrings, so training can be done classically, while sampling from the circuit's output distribution is the part delegated to quantum hardware. The tensor-network simulation exploits the fact that each ansatz layer is a matrix-product operator of bond dimension 2, making exact contraction linear in qubit count for the two-layer circuits used.
What would settle it
Run the same mRNA sequences through the two workflows many times, then compare every final post-processed bitstring against the exact optimum found by a classical exhaustive solver for instances up to 156 qubits; if the post-processed hit rate is far below the paper's reported results, the optimization claim is falsified. Separately, take the optimal QUBO bitstrings for a panel of mRNAs with experimentally known structures and compare the predicted base pairs to the measured ones; if the agreement is no better than chance, the biological motivation is falsified even though the optimization succeeded.
Extended reading notes
Core claim
On its own terms, the paper's discovery is that hybrid quantum-classical optimization can solve the specific QUBO instances derived from mRNA folding to proven optimality, not merely to good approximate energies. For the CVaR-based workflow, 133- and 150-qubit instances from 60- and 48-nucleotide mRNAs were run on real quantum processors, and for the IQP-based workflow, 127- and 156-qubit instances from 45- and 60-nucleotide mRNAs; after the classical local-search post-processing, the exact optimal objective values were found. In noiseless tensor-network simulations of the same CVaR algorithm, the method tracked the optimum up to 354 qubits, sometimes only after resuming from the best parameter configuration seen in an epoch, and the relative error of the best samples grew with system size. The paper presents this as evidence that the practical capability of quantum-centric methods for large biological optimization problems is growing, while being explicit that no performance guarantees follow from the heuristic nature of the schemes.
Load-bearing premise
The biological meaning of the whole exercise rests on one unvalidated premise: that the quartet QUBO with empirical nearest-neighbor energies and the chosen penalty weights is a faithful model of real mRNA secondary structure, and the paper never checks its predicted foldings against experimentally determined RNA structures.
Editorial extensions
If this is right
- For mRNA sequences up to 60 nucleotides, the demonstrated recipes give a path to certified optimal QUBO solutions with roughly 156 qubits and up to 950 nonlocal gates, roughly doubling the 80-qubit / 42-nucleotide scale previously reported.
- The noiseless tensor-network results support the claim that the CVaR workflow can operate at 354 qubits, so the practical ceiling for longer sequences is set mainly by hardware noise and the expressivity of the shallow ansatz, not by the optimization principle.
- The IQP scheme can be run with fully classical training, meaning the expensive variational loop is moved off the quantum processor and the hardware's role is reduced to sampling a fixed optimized circuit.
- The gauge-transformation plus parameter-threshold plus local-search post-processing stack is independent of the specific mRNA instance and should transfer directly to other dense QUBO problems whose optima are low-Hamming-weight bitstrings.
Reading between the lines
- Because optimality is certified only against the QUBO objective, a natural next test is to score the same optimal bitstrings against experimentally characterized mRNA structures; if systematic mismatches appear, the energy coefficients or penalty weights in Eq. (2) would need retuning rather than the quantum pipeline.
- The bounded improvement of the local search means the real benchmark for these workflows is the distance between the mitigated quantum samples and the optimum; a useful extension would probe whether stronger gauge selection or shallower circuits shrink that distance at 300 or more qubits.
- The IQP route's classical trainability raises a spoofing question the paper does not answer: if a classical sampler can mimic the mitigated output distribution, the quantum sampling step would be redundant. Comparing quantum hardware samples with classical samples from the same optimized IQP circuit would settle that empirically.
- The variable-reduction scheme the paper uses to shrink 256-variable problems to 133 or 156 qubits is itself a transferable tool; applying it to other high-edge-density QUBOs could make the quantum-centric template useful beyond RNA folding.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper proposes two quantum-centric workflows for solving QUBO formulations of mRNA secondary structure prediction: a CVaR-based variational algorithm enhanced with gauge transformations, parameter thresholding, and classical local search, and a classically trained IQP circuit whose optimized parameters are sampled on quantum hardware with subsequent error mitigation and local search. The authors report hardware experiments on IBM processors with 127-156 qubits, tensor-network simulations up to 406 qubits, and CPLEX-verified optimal solutions for several reduced instances. An appendix describes a variable-reduction scheme used to map 256-variable problems down to 133/150/156-qubit instances, and the stated claim is that mRNA sequences of up to 60 nucleotides can be tackled at this scale.
Significance. If the optimization claims hold, this is a useful engineering demonstration of hybrid quantum-classical optimization on utility-scale hardware, with practical details (gauge transformations, parameter thresholding, IQP expectation-based training, and an exact MPS contraction scheme) that could inform future work. The paper provides machine-checkable CPLEX verification of the reduced instances and reproducible algorithmic descriptions. However, the significance is currently limited by an unsound reduction proof, the absence of classical baselines, and an internal inconsistency in the tensor-network scalability results; these issues must be resolved before the central claims about 'solving' 60-nucleotide mRNA problems can be accepted.
major comments (4)
- [Appendix A, Eq. (3) and preceding paragraph] The reduction scheme is not exact, and the proof given is internally inconsistent. The paper first claims that variables in κ 'contributions to Q will always be ≥ 0' because their quadratic coefficients are nonnegative, but this ignores negative linear coefficients h_i; two sentences later it concedes that variables with h_i < 0 can lower Qκ. A concrete counterexample satisfying the paper's own condition |h_i|≪|J_ij| is: h_z = -1, h_y = -2, J_zy = 100, with y∈κ and z∉κ. Solving Qred over z yields z=1 with value -1; optimizing κ with z fixed gives y=0 and total -1, but the true optimum of the full QUBO is z=0, y=1 with value -2. Since the 133/150/156-qubit hardware instances are obtained by applying this reduction to 256-variable problems, the CPLEX-verified optima and the claimed '60-nucleotide' results are for the reduced QUBO, not for the original mRNA problem. The authors must prove exactness under the stated assumptions (which the counterexample shows is impossible without additional restrictions), verify the original instances with CPLEX or another exact solver, or explicitly re-scope the claims to the reduced problems.
- [Section III-A.4 and Section III-C.1, Figs. 4 and 5] No classical baseline is reported on the same instances. The paper does not state how often the local-search post-processing alone (from random or trivial starting bitstrings, or from classically simulated samples) reaches the CPLEX-verified optimum, nor does it compare the hardware samples with samples drawn classically from the same trained distribution. Without such an ablation, the specific contribution of the quantum processor to the claimed 'solving' of these instances is not established.
- [Section III-B.2 and Table I] There is an internal inconsistency in the tensor-network scalability claim. The text states that 'Applying this strategy, we successfully solve the 354-qubit problem instance,' but Table I reports 0 hits out of 100 for 354 qubits both without and with post-processing, with relative errors of 21.4% and 10.5%. If the table refers to a baseline before the resume-from-best-parameter strategy, this must be stated clearly; otherwise the reported simulation results contradict the table.
- [Section II, Eq. (2); Section IV] The manuscript does not validate the QUBO model as a predictor of mRNA secondary structure. No comparison is made to experimentally determined structures or to standard classical predictors (e.g., ViennaRNA) on the same sequences, and no discussion of the mapping from a QUBO optimum to an actual secondary structure is provided. The title and abstract claim 'secondary structure prediction,' but the demonstrated results are solutions to a QUBO whose biological fidelity is unexamined. The authors should either add structural validation or explicitly limit the paper's claims to QUBO optimization.
minor comments (6)
- [Fig. 5 caption] The caption says '127 and 150 qubit problems' and 'optimal objective values of -161.5 and -249.1 for the 127 and 150 qubit problems respectively,' but the text and panel (c) describe a 156-qubit problem; the caption should be corrected.
- [Section III-A.4] The mapping of sequence lengths to qubit counts is confusing: the 133-qubit and 150-qubit problems are said to originate from sequences of length 60 and 48, while the 156-qubit IQP problem is said to come from a 60-nucleotide sequence. Clarify which sequence is used for each experiment and why the reduced sizes differ so much for the same sequence length.
- [Section III-B.2, Table I] The table reports γ as 'relative error' but the definition in the text (|F(θf)_low - F0| / |F0|) is for the lowest value over all samples at any time; clarify whether the table entries for the 'no post-processing' column use raw samples or the best parameter configuration over the run.
- [Section III-A.3, Algorithm 1] The sentence 'for j in Permute(x)' should be 'for j in Permute({1,...,n})' to be precise. Also, the bound Δ = 2(Σ_i h_i + Σ_{(i,j)∈G} J_{ij}) for the maximum decrease of the local search is incorrect when h_i or J_{ij} are negative; for a starting all-zero bitstring with negative h_i and positive J_{ij}, the bound can be negative while the attainable decrease is nonnegative.
- [Section III-C] The phrase 'the expectation calculation ... consists of computing averages over bit strings generated randomly from a uniform distribution' should be more explicit that this is a classical Monte Carlo estimate using finitely many samples (2^15), not an exact evaluation; the approximation error is not discussed.
- [References] Reference [28] has an incomplete title ('Does provable absence of barren plateaus imply classical simulability, Or, why we need to rethink variational quantum computing'); also, the paper's claims about 'classically difficult' IQP sampling should acknowledge the noisy-regime caveat more prominently than the single reference to Ref. [43].
Circularity Check
No significant circularity found; central optima are benchmarked against external CPLEX solutions.
full rationale
The claimed derivations are self-contained rather than circular. The central optimization target is the QUBO of Eq. (2), whose coefficients come from empirical nearest-neighbor thermodynamic parameters (Ref. [48]) and constraint penalties; no quantity in that objective is fitted from the hardware samples or from CPLEX outputs. Both workflows minimize the same Hamiltonian: the CVaR VQA uses hardware samples to update parameters against Hp, and the IQP scheme trains classically on expectation values of Hp and then samples the optimized circuit. The ground-truth optimum used for judging success is computed by CPLEX, an external classical solver, so the reported solutions are not defined in terms of the algorithms' own outputs. Self-citations to Ref. [11] (earlier mRNA QUBO/VQA work) and Refs. [44,45] (IQP expectation optimization) are methodological and are not used as an unverified uniqueness theorem or as the sole justification of the central claim. The Appendix A variable-reduction step is a mathematical reduction of the QUBO; whether its proof is fully sound is a correctness concern, not a circularity, because the reduced problem is not being equated to the original by any self-referential construction. There is no fitted parameter renamed as a prediction and no load-bearing self-citation chain. Hence a score of 0 is appropriate.
Assumptions & free parameters
free parameters (6)
- CVaR tail parameter alpha =
0.2
- Gauge selection threshold p_th =
0.8
- Parameter threshold theta_th =
0.06
- IQP mitigation threshold <Z_i>_th =
0.99
- Ansatz depth p =
2
- QUBO reward and penalty coefficients r, p, t =
not stated in text
assumptions (6)
- domain assumption The quartet QUBO in Eq. (2) accurately represents mRNA secondary structure prediction within the nearest-neighbor model.
- domain assumption Each base can pair at most once and crossing quartets are forbidden through the penalties in Eq. (2).
- ad hoc to paper The optimal QUBO bitstring has low Hamming weight, so gauge transformations can map noisy high-weight samples toward the optimum.
- ad hoc to paper Hardware noise predominantly flips 0 to 1, so single-qubit expectation values below p_th identify noisy qubits.
- standard math The tensor-network MPS with bond dimension 2^p exactly represents the p-layer circuit used here.
- standard math IQP expectation values can be computed classically in polynomial time for the Hamiltonians used.
Cite this review
Pith. "Pith review of Towards secondary structure prediction of longer mRNA sequences using a quantum-centric optimization scheme." pith.science (2026). https://pith.science/paper/3X22A6UN
@misc{pith2026250505782,
author = {Pith},
title = {Pith review of: Towards secondary structure prediction of longer mRNA sequences using a quantum-centric optimization scheme},
year = {2026},
howpublished = {\url{https://pith.science/paper/3X22A6UN}},
note = {Machine review of arXiv:2505.05782}
}
read the original abstract
Accurate prediction of mRNA secondary structure is critical for understanding gene expression, translation efficiency, and advancing mRNA-based therapeutics. However, the combinatorial complexity of possible foldings, especially in long sequences, poses significant computational challenges for classical algorithms. In this work, we propose a scalable, quantum-centric optimization framework that integrates quantum sampling with classical post-processing to tackle this problem. Building on a Quadratic Unconstrained Binary Optimization (QUBO) formulation of the mRNA folding task, we develop two complementary workflows: a Conditional Value at Risk (CVaR)-based variational quantum algorithm enhanced with gauge transformations and local search, and an Instantaneous Quantum Polynomial (IQP) circuit-based scheme where training is done classically and sampling is delegated to quantum hardware. We demonstrate the effectiveness of these approaches using IBM quantum processors, solving problem instances with up to 156 qubits and circuits containing up to 950 nonlocal gates, corresponding to mRNA sequences of up to 60 nucleotides. Additionally, we validate scalability of the CVaR algorithm on a tensor network simulator, reaching up to 354 qubits in noiseless settings. These results demonstrate the growing practical capabilities of hybrid quantum-classical methods for tackling large-scale biological optimization problems.
Figures
Figures from the paper (2 more)
Reference graph
Works this paper leans on
-
[1]
Thoughts on how to think (and talk) about RNA structure,
Q. Vicens and J. S. Kieft, “Thoughts on how to think (and talk) about RNA structure,” Proceedings of the National Academy of Sciences , vol. 119, no. 17, p. e2112677119, 2022
work page 2022
-
[2]
Tailor made: the art of therapeutic mRNA design,
M. Metkar, C. S. Pepin, and M. J. Moore, “Tailor made: the art of therapeutic mRNA design,” Nature Reviews Drug Discovery , vol. 23, no. 1, pp. 67–83, 2024
2024
-
[3]
mRNA-based therapeutics: powerful and versatile tools to combat diseases,
S. Qin, X. Tang, Y . Chen, K. Chen, N. Fan, W. Xiao, Q. Zheng, G. Li, Y . Teng, M. Wu et al., “mRNA-based therapeutics: powerful and versatile tools to combat diseases,” Signal Transduction and Targeted Therapy, vol. 7, no. 1, p. 166, 2022
work page 2022
-
[4]
Predicting rna structures and functions by artificial intelligence,
J. Zhang, M. Lang, Y . Zhou, and Y . Zhang, “Predicting rna structures and functions by artificial intelligence,” Trends in Genetics , 2024
work page 2024
-
[5]
RNA pseudoknot prediction in energy-based models,
R. B. Lyngsø and C. N. Pedersen, “RNA pseudoknot prediction in energy-based models,” Journal of Computational Biology , vol. 7, no. 3-4, pp. 409–427, 2000
work page 2000
-
[6]
Computer prediction of RNA structure,
M. Zuker, “Computer prediction of RNA structure,” in Methods in enzymology. Elsevier, 1989, vol. 180, pp. 262–288
work page 1989
-
[7]
Mfold web server for nucleic acid folding and hybridization prediction,
M. Zuker, “Mfold web server for nucleic acid folding and hybridization prediction,” Nucleic Acids Research , vol. 31, no. 13, pp. 3406–3415, 2003
work page 2003
-
[8]
RNA structures and folding: from conventional to new issues in structure predictions,
P. Schuster, P. F. Stadler, and A. Renner, “RNA structures and folding: from conventional to new issues in structure predictions,” Current Opinion in Structural Biology , vol. 7, no. 2, pp. 229–235, 1997
work page 1997
Show all 63 references
-
[9]
Infernal 1.1: 100-fold faster RNA homology searches,
E. P. Nawrocki and S. R. Eddy, “Infernal 1.1: 100-fold faster RNA homology searches,” Bioinformatics, vol. 29, no. 22, pp. 2933–2935, 2013
2013
-
[10]
Rich parame- terization improves RNA structure prediction,
S. Zakov, Y . Goldberg, M. Elhadad, and M. Ziv-Ukelson, “Rich parame- terization improves RNA structure prediction,”Journal of Computational Biology, vol. 18, no. 11, pp. 1525–1542, 2011
2011
-
[11]
mrna secondary structure prediction using utility-scale quantum computers,
D. Alevras, M. Metkar, T. Yamamoto, V . Kumar, T. Friedhoff, J.- E. Park, M. Takeori, M. LaDue, W. Davis, and A. Galda, “mrna secondary structure prediction using utility-scale quantum computers,” in 2024 IEEE International Conference on Quantum Computing and Engineering (QCE)...
2024
-
[12]
Advances in rna secondary structure prediction and rna modifications: Methods, data, and applications,
S. Yang, N. T. Pham, Z. Li, J. Y . Baik, J. Lee, T. Zhai, W. Yu, B. Hou, T. Shang, W. He et al., “Advances in rna secondary structure prediction and rna modifications: Methods, data, and applications,” arXiv preprint arXiv:2501.04056, 2025
2025 arXiv
-
[13]
Provable bounds for noise-free ex- pectation values computed from noisy samples,
S. V . Barron, D. J. Egger, E. Pelofske, A. B ¨artschi, S. Eidenbenz, M. Lehmkuehler, and S. Woerner, “Provable bounds for noise-free ex- pectation values computed from noisy samples,” Nature Computational Science, pp. 1–11, 2024
2024
-
[14]
Benchmarking digital quantum simulations and optimization above hundreds of qubits using quantum critical dynamics,
A. Miessen, D. J. Egger, I. Tavernelli, and G. Mazzola, “Benchmarking digital quantum simulations and optimization above hundreds of qubits using quantum critical dynamics,” arXiv preprint arXiv:2404.08053 , 2024
2024 arXiv
-
[15]
Large-scale quantum approximate opti- mization on nonplanar graphs with machine learning noise mitigation,
S. H. Sack and D. J. Egger, “Large-scale quantum approximate opti- mization on nonplanar graphs with machine learning noise mitigation,” Physical Review Research , vol. 6, no. 1, p. 013223, 2024
2024
-
[16]
Quantum optimization using a 127-qubit gate-model ibm quantum computer can outperform quantum annealers for nontrivial binary optimization problems,
N. Sachdeva, G. S. Hartnett, S. Maity, S. Marsh, Y . Wang, A. Winick, R. Dougherty, D. Canuto, Y . Q. Chong, M. Hush et al. , “Quantum optimization using a 127-qubit gate-model ibm quantum computer can outperform quantum annealers for nontrivial binary optimization problems,” ...
2024 arXiv
-
[17]
Bias-field digitized counterdiabatic quantum algorithm for higher-order binary optimization,
S. V . Romero, A.-M. Visuri, A. G. Cadavid, E. Solano, and N. N. Hegade, “Bias-field digitized counterdiabatic quantum algorithm for higher-order binary optimization,” arXiv preprint arXiv:2409.04477 , 2024
2024 arXiv
-
[18]
Scaling the variational quantum eigensolver for dy- namic portfolio optimization,
´A. Nodar, I. De Le ´on, D. Arias, E. Mamedaliev, M. E. Molina, M. Mart ´ın-Cordero, S. Hern ´andez-Santana, P. Serrano, M. Arranz, O. Mentxaka et al., “Scaling the variational quantum eigensolver for dy- namic portfolio optimization,” arXiv preprint arXiv:2412.19150 , 2024
2024 arXiv
-
[19]
Bias- field digitized counterdiabatic quantum optimization,
A. G. Cadavid, A. Dalal, A. Simen, E. Solano, and N. N. Hegade, “Bias- field digitized counterdiabatic quantum optimization,” arXiv preprint arXiv:2405.13898, 2024
2024 arXiv
-
[20]
Im- proving quantum approximate optimization by noise-directed adaptive remapping,
F. B. Maciejewski, J. Biamonte, S. Hadfield, and D. Venturelli, “Im- proving quantum approximate optimization by noise-directed adaptive remapping,” arXiv preprint arXiv:2404.01412 , 2024
2024
-
[21]
Implementing transferable annealing protocols for combinatorial opti- mization on neutral-atom quantum processors: A case study on smart charging of electric vehicles,
L. Leclerc, C. Dalyac, P. Bendotti, R. Griset, J. Mikael, and L. Henriet, “Implementing transferable annealing protocols for combinatorial opti- mization on neutral-atom quantum processors: A case study on smart charging of electric vehicles,” Physical Review A , vol. 111, no....
2025
-
[22]
Training variational quantum algorithms is np-hard,
L. Bittel and M. Kliesch, “Training variational quantum algorithms is np-hard,” Physical review letters , vol. 127, no. 12, p. 120502, 2021
2021
-
[23]
Non- trivial symmetries in quantum landscapes and their resilience to quantum noise,
E. Fontana, M. Cerezo, A. Arrasmith, I. Rungger, and P. J. Coles, “Non- trivial symmetries in quantum landscapes and their resilience to quantum noise,” Quantum, vol. 6, p. 804, 2022
2022
-
[24]
Quantum variational algorithms are swamped with traps,
E. R. Anschuetz and B. T. Kiani, “Quantum variational algorithms are swamped with traps,” Nature Communications, vol. 13, no. 1, p. 7760, 2022
2022
-
[25]
Diagnosing barren plateaus with tools from quantum optimal control,
M. Larocca, P. Czarnik, K. Sharma, G. Muraleedharan, P. J. Coles, and M. Cerezo, “Diagnosing barren plateaus with tools from quantum optimal control,” Quantum, vol. 6, p. 824, 2022
2022
-
[26]
Barren plateaus in quantum neural network training landscapes,
J. R. McClean, S. Boixo, V . N. Smelyanskiy, R. Babbush, and H. Neven, “Barren plateaus in quantum neural network training landscapes,”Nature communications, vol. 9, no. 1, p. 4812, 2018
2018
-
[27]
A review of barren plateaus in variational quantum computing,
M. Larocca, S. Thanasilp, S. Wang, K. Sharma, J. Biamonte, P. J. Coles, L. Cincio, J. R. McClean, Z. Holmes, and M. Cerezo, “A review of barren plateaus in variational quantum computing,” arXiv preprint arXiv:2405.00781, 2024
2024 arXiv
-
[28]
Does provable absence of barren plateaus imply classical simulability,
M. Cerezo, M. Larocca, D. Garc ´ıa-Mart´ın, N. Diaz, P. Braccia, E. Fontana, M. S. Rudolph, P. Bermejo, A. Ijaz, S. Thanasilp et al. , “Does provable absence of barren plateaus imply classical simulability,” Or , why we need to rethink variational quantum computing , 2023
2023
-
[29]
Circuit depth versus energy in topologically ordered systems,
A. Tikku and I. H. Kim, “Circuit depth versus energy in topologically ordered systems,” arXiv preprint arXiv:2210.06796 , 2022
2022 arXiv
-
[30]
Chem- istry beyond exact solutions on a quantum-centric supercomputer,
J. Robledo-Moreno, M. Motta, H. Haas, A. Javadi-Abhari, P. Jurcevic, W. Kirby, S. Martiel, K. Sharma, S. Sharma, T. Shirakawaet al., “Chem- istry beyond exact solutions on a quantum-centric supercomputer,” arXiv preprint arXiv:2405.05068, 2024
2024 arXiv
-
[31]
Accurate quantum- centric simulations of supramolecular interactions,
D. Kaliakin, A. Shajan, J. R. Moreno, Z. Li, A. Mitra, M. Motta, C. Johnson, A. A. Saki, S. Das, I. Sitdikov et al. , “Accurate quantum- centric simulations of supramolecular interactions,” arXiv preprint arXiv:2410.09209, 2024
-
[32]
Improving variational quantum optimization using cvar,
P. K. Barkoutsos, G. Nannicini, A. Robert, I. Tavernelli, and S. Woerner, “Improving variational quantum optimization using cvar,” Quantum, vol. 4, p. 256, 2020
2020
-
[33]
The density-matrix renormalization group in the age of matrix product states,
U. Schollw ¨ock, “The density-matrix renormalization group in the age of matrix product states,” Annals of physics , vol. 326, no. 1, pp. 96–192, 2011
2011
-
[34]
Tensor network quantum simulator with step-dependent parallelization,
D. Lykov, R. Schutski, A. Galda, V . Vinokur, and Y . Alexeev, “Tensor network quantum simulator with step-dependent parallelization,” in 2022 IEEE International Conference on Quantum Computing and Engineer- ing (QCE) . IEEE, 2022, pp. 582–593
2022
-
[35]
A practical introduction to tensor networks: Matrix product states and projected entangled pair states,
R. Or ´us, “A practical introduction to tensor networks: Matrix product states and projected entangled pair states,” Annals of physics , vol. 349, pp. 117–158, 2014
2014
-
[36]
What limits the simulation of quantum computers?
Y . Zhou, E. M. Stoudenmire, and X. Waintal, “What limits the simulation of quantum computers?” Physical Review X , vol. 10, no. 4, p. 041038, 2020
2020
-
[37]
Density-matrix renormalization group algorithm for sim- ulating quantum circuits with a finite fidelity,
T. Ayral, T. Louvet, Y . Zhou, C. Lambert, E. M. Stoudenmire, and X. Waintal, “Density-matrix renormalization group algorithm for sim- ulating quantum circuits with a finite fidelity,” PRX Quantum , vol. 4, no. 2, p. 020304, 2023
2023
-
[38]
Permutational quantum computing,
S. P. Jordan, “Permutational quantum computing,” arXiv preprint arXiv:0906.2508, 2009
2009 arXiv
-
[39]
Quantum complexity: restrictions on algorithms and architectures,
D. J. Shepherd, “Quantum complexity: restrictions on algorithms and architectures,” arXiv preprint arXiv:1005.1425 , 2010
2010 arXiv
-
[40]
Classical simulation of commuting quantum computations implies collapse of the polynomial hierarchy,
M. J. Bremner, R. Jozsa, and D. J. Shepherd, “Classical simulation of commuting quantum computations implies collapse of the polynomial hierarchy,” Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences , vol. 467, no. 2126, pp. 459–472, 2011
2011
-
[41]
Average-case complexity versus approximate simulation of commuting quantum com- putations,
M. J. Bremner, A. Montanaro, and D. J. Shepherd, “Average-case complexity versus approximate simulation of commuting quantum com- putations,” Physical review letters , vol. 117, no. 8, p. 080501, 2016
2016
-
[42]
Improved separation between quantum and classical computers for sampling and functional tasks,
S. C. Marshall, S. Aaronson, and V . Dunjko, “Improved separation between quantum and classical computers for sampling and functional tasks,” arXiv preprint arXiv:2410.20935 , 2024
2024 arXiv
-
[43]
Rajakumar, J
J. Rajakumar, J. D. Watson, and Y .-K. Liu, Polynomial-Time Classical Simulation of Noisy IQP Circuits with Constant Depth . Society for Industrial and Applied Mathematics, Jan. 2025, p. 1037–1056. ISBN 9781611978322. [Online]. Available: http://dx.doi.org/10.1137/1. 9781611978322.30
2025 doi
-
[44]
Iqpopt: Fast optimization of instantaneous quantum polynomial circuits in jax,
E. Recio-Armengol and J. Bowles, “Iqpopt: Fast optimization of instantaneous quantum polynomial circuits in jax,” arXiv preprint arXiv:2501.04776, 2025
2025 arXiv
-
[45]
Train on classical, deploy on quantum: scaling generative quantum machine learning to a thousand qubits,
E. Recio-Armengol, S. Ahmed, and J. Bowles, “Train on classical, deploy on quantum: scaling generative quantum machine learning to a thousand qubits,” arXiv preprint arXiv:2503.02934 , 2025
2025
-
[46]
Gusfield, Integer Linear Programming in Computational and Systems Biology: An Entry-Level Text and Course
D. Gusfield, Integer Linear Programming in Computational and Systems Biology: An Entry-Level Text and Course . Cambridge University Press, 2019
2019
-
[47]
A tutorial on formulating and using qubo models,
F. Glover, G. Kochenberger, and Y . Du, “A tutorial on formulating and using qubo models,” arXiv preprint arXiv:1811.11538 , 2018
2018 arXiv
-
[48]
NNDB: the nearest neighbor parameter database for predicting stability of nucleic acid secondary structure,
D. H. Turner and D. H. Mathews, “NNDB: the nearest neighbor parameter database for predicting stability of nucleic acid secondary structure,” Nucleic Acids Research, vol. 38, no. suppl 1, p. D280– D282, 2009
2009
-
[49]
Qiskit: An open-source framework for quantum computing,
Qiskit contributors, “Qiskit: An open-source framework for quantum computing,” 2023
2023
-
[50]
Optimizing the spin reversal transform on the d-wave 2000q,
E. Pelofske, G. Hahn, and H. Djidjev, “Optimizing the spin reversal transform on the d-wave 2000q,” in 2019 IEEE International Conference on Rebooting Computing (ICRC) . IEEE, 2019, pp. 1–8
2019
-
[51]
Optimizing embedding-related quantum annealing parameters for reducing hardware bias,
A. Barbosa, E. Pelofske, G. Hahn, and H. N. Djidjev, “Optimizing embedding-related quantum annealing parameters for reducing hardware bias,” in Parallel Architectures, Algorithms and Programming: 11th International Symposium, PAAP 2020, Shenzhen, China, December 28– 30, 2020, ...
2020
-
[52]
Sequential minimal optimiza- tion for quantum-classical hybrid algorithms,
K. M. Nakanishi, K. Fujii, and S. Todo, “Sequential minimal optimiza- tion for quantum-classical hybrid algorithms,” Phys. Rev. Res. , vol. 2, p. 043158, Oct 2020. doi: 10.1103/PhysRevResearch.2.043158
2020 doi
-
[53]
Evaluating the impact of noise on the performance of the variational quantum eigensolver,
M. Oliv, A. Matic, T. Messerer, and J. M. Lorenz, “Evaluating the impact of noise on the performance of the variational quantum eigensolver,” arXiv preprint arXiv:2209.12803 , 2022
2022 arXiv
-
[54]
Towards large-scale quantum optimiza- tion solvers with few qubits,
M. Sciorilli, L. Borges, T. L. Patti, D. Garc ´ıa-Mart´ın, G. Camilo, A. Anandkumar, and L. Aolita, “Towards large-scale quantum optimiza- tion solvers with few qubits,” Nature Communications , vol. 16, no. 1, p. 476, 2025
2025
-
[55]
Glover and M
F. Glover and M. Laguna, Tabu search. Springer, 1998
1998
-
[56]
Finitely correlated states on quantum spin chains,
M. Fannes, B. Nachtergaele, and R. F. Werner, “Finitely correlated states on quantum spin chains,” Communications in mathematical physics , vol. 144, pp. 443–490, 1992
1992
-
[57]
Thermodynamic limit of density matrix renormalization,
S. ¨Ostlund and S. Rommer, “Thermodynamic limit of density matrix renormalization,” Physical review letters, vol. 75, no. 19, p. 3537, 1995
1995
-
[58]
Efficient classical simulation of slightly entangled quantum computations,
G. Vidal, “Efficient classical simulation of slightly entangled quantum computations,” Physical review letters, vol. 91, no. 14, p. 147902, 2003
2003
-
[59]
Guidable local hamiltonian problems with implications to heuristic ansatz state preparation and the quantum pcp conjecture,
J. Weggemans, M. Folkertsma, and C. Cade, “Guidable local hamiltonian problems with implications to heuristic ansatz state preparation and the quantum pcp conjecture,” in 19th Conference on the Theory of Quantum Computation, Communication and Cryptography , 2024
2024
-
[60]
Non-zero noise extrapolation: accurately simulating noisy quantum circuits with tensor networks,
A. P. Thompson, A. Soeteman, C. Cade, and I. Niesen, “Non-zero noise extrapolation: accurately simulating noisy quantum circuits with tensor networks,” arXiv preprint arXiv:2501.13237 , 2025
2025
-
[61]
Simulating quantum computers with probabilistic methods,
M. Nest, “Simulating quantum computers with probabilistic methods,” arXiv preprint arXiv:0911.1624 , 2009
2009 arXiv
-
[62]
Quantum algorithms for fixed qubit architectures,
E. Farhi, J. Goldstone, S. Gutmann, and H. Neven, “Quantum algorithms for fixed qubit architectures,” arXiv preprint arXiv:1703.06199 , 2017
2017 arXiv
-
[63]
Quantum-enhanced markov chain monte carlo,
D. Layden, G. Mazzola, R. V . Mishmash, M. Motta, P. Wocjan, J.-S. Kim, and S. Sheldon, “Quantum-enhanced markov chain monte carlo,” Nature, vol. 619, no. 7969, pp. 282–287, 2023
2023
Reviewed August 15, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.