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arxiv: 2605.08332 · v1 · submitted 2026-05-08 · 🪐 quant-ph · cs.AI

Recognition: 2 theorem links

· Lean Theorem

Optimal FALQON for Quantum Approximate Optimization via Layer-wise Parameter Tuning

Authors on Pith no claims yet

Pith reviewed 2026-05-12 01:03 UTC · model grok-4.3

classification 🪐 quant-ph cs.AI
keywords FALQONquantum approximate optimizationcombinatorial optimizationNISQ deviceslayer-wise parameter optimizationQAOA warm-startfeedback-based quantum optimization
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The pith

Optimizing per-layer time steps and scaling factors in FALQON improves success probability and efficiency for combinatorial optimization on quantum devices.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper aims to show that standard FALQON can be enhanced by treating its per-layer time step and scaling factor as variables to be optimized classically rather than fixed in advance. This matters because the original method often needs hundreds or thousands of layers to reach good solutions, limiting its usefulness on current quantum hardware. The authors test this on all 94 non-isomorphic 3-regular graphs with 12 vertices and find statistically significant gains in success rates, fewer evaluations needed, and lower depth-normalized costs compared to standard FALQON and some QAOA versions. They also show that these optimized parameters provide better starting points for QAOA. If correct, this makes feedback-based quantum optimization more practical by reducing circuit depth requirements.

Core claim

Optimal FALQON formulates the per-layer parameters δ_k and M_k as decision variables that are optimized classically at each step, leading to faster convergence and higher success probabilities than fixed-parameter FALQON on small 3-regular graphs.

What carries the argument

The layer-wise classical optimization of the time step δ_k and scaling factor M_k, which replaces the fixed hyperparameters of standard FALQON.

Load-bearing premise

That the classical optimization of per-layer parameters remains computationally feasible and that performance gains observed on 12-vertex graphs will hold for larger or different problem instances.

What would settle it

Observing whether the success probability improvements persist when applied to graphs with 20 or more vertices, or whether the classical optimization time exceeds the quantum evaluation savings.

Figures

Figures reproduced from arXiv: 2605.08332 by Michael Mancini, Shabnam Sodagari.

Figure 1
Figure 1. Figure 1: Depth-wise distributions of Psuccess for FALQON family. Optimal FALQON medians consistently exceed standard FALQON across all depths, with pronounced separation at higher depths. 1 2 3 4 5 6 7 8 9 10 Depth (Layers) 0.000 0.001 0.002 0.003 0.004 0.005 E1 = Psuccess nevals E1 = Psuccess nevals (FALQON) Method FALQON FO Optimal FALQON FO (Ours) FALQON SO Optimal FALQON SO (Ours) [PITH_FULL_IMAGE:figures/full… view at source ↗
Figure 2
Figure 2. Figure 2: Depth-wise distributions of E1 for FALQON variants. Optimal FALQON demonstrates median evaluation-normalized efficiency approximately 5-50 times higher than standard FALQON. requires stronger initialization guidance to avoid poor local minima. Warm-starting from Optimal FALQON dramatically improves performance: median success probability rises from ∼ 0.002 (fixed) and ∼ 0.007 (warm-start from standard FALQ… view at source ↗
Figure 3
Figure 3. Figure 3: Depth-wise distributions of E2 for FALQON variants. Optimal FALQON retains median efficiency advantage after joint evaluation-depth normalization, indicating genuine adaptive benefits. 1 2 3 4 5 6 7 8 9 10 Depth (Layers) 0.0 0.2 0.4 0.6 0.8 Psuccess Psuccess (QAOA (Gradient Descent)) Method QAOA (GD) Warm-Start FALQON FO QAOA (GD) Warm-Start Optimal FALQON FO QAOA (GD) (Ours) Warm-Start FALQON SO QAOA (GD)… view at source ↗
Figure 4
Figure 4. Figure 4: Depth-wise Psuccess for QAOA with gradient descent. Warm-starting from Optimal FALQON shifts distributions upward relative to fixed initialization and standard FALQON warm-starts. (fixed init) and ∼ 0.003 (warm start from standard FALQON) to ∼ 0.27 (warm start from Optimal FALQON). F. Efficiency Metrics and Cost Analysis [PITH_FULL_IMAGE:figures/full_fig_p006_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: Depth-wise Psuccess for QAOA with Powell optimizer. Warm-start from Optimal FALQON dominates at most depths; fixed QAOA competitive at isolated depths. 1 2 3 4 5 6 7 8 9 10 Depth (Layers) 0.0 0.2 0.4 0.6 0.8 Psuccess Psuccess (QAOA-MA (Gradient Descent)) Method QAOA-MA (GD) Warm-Start FALQON FO QAOA-MA (GD) Warm-Start Optimal FALQON FO QAOA-MA (GD) (Ours) Warm-Start FALQON SO QAOA-MA (GD) Warm-Start Optima… view at source ↗
Figure 6
Figure 6. Figure 6: Depth-wise Psuccess for QAOA-MA with gradient descent. Warm-start from Optimal FALQON shows pronounced advantage over fixed initialization and standard FALQON warm-starts. superior E1 at depths L = 2 and L = 10, revealing depth-dependent efficiency tradeoffs. This suggests that fixed initialization may be sufficient, and further investigations com￾paring QAOA with and without Optimal FALQON warm start sche… view at source ↗
Figure 7
Figure 7. Figure 7: Depth-wise Psuccess for QAOA-MA with Powell optimizer, demonstrating our method’s effectiveness. 1 2 3 4 5 6 7 8 9 10 Depth (Layers) 0.000 0.002 0.004 0.006 0.008 E1 = Psuccess nevals E1 = Psuccess nevals (QAOA (Powell)) Method QAOA (Powell) Warm-Start FALQON FO QAOA (Powell) Warm-Start Optimal FALQON FO QAOA (Powell) (Ours) Warm-Start FALQON SO QAOA (Powell) Warm-Start Optimal FALQON SO QAOA (Powell) (Our… view at source ↗
Figure 8
Figure 8. Figure 8: Depth-wise E1 efficiency for QAOA (Powell). Optimal FALQON warm-starts maintain high efficiency at most depths; fixed QAOA competitive at L = 2, 10. 0.22 compared to standard FALQON’s ∼ 0.004 (50× im￾provement). In evaluation-normalized efficiency E1, Opti￾mal FALQON reaches 1.35–1.68 × 10−3 versus standard FALQON’s 0.07–0.32 × 10−3 (4–23× improvement). For depth-aware efficiency E2, Optimal FALQON achieve… view at source ↗
read the original abstract

Feedback-based adaptive quantum optimization (FALQON) is a promising approach for solving combinatorial problems on noisy intermediate-scale quantum (NISQ) devices, requiring only single circuit evaluations per layer. However, standard FALQON relies on fixed hyperparameters that severely limit convergence speed, requiring hundreds to thousands of layers for acceptable solutions. This paper proposes Optimal FALQON, an optimization-based formulation that treats the per-layer time step ($\delta_k$) and scaling factor ($M_k$) as decision variables optimized via classical methods. We present a comprehensive empirical study on all 94 non-isomorphic 3-regular graphs with 12 vertices, comparing Optimal FALQON with standard FALQON and multiple QAOA variants. Results demonstrate statistically significant improvements in success probability, evaluation efficiency, and depth-normalized cost across the evaluated benchmarks. Furthermore, initializing QAOA with parameters from Optimal FALQON yields superior warm-start performance compared to fixed initialization.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

3 major / 2 minor

Summary. The manuscript introduces Optimal FALQON, which treats the per-layer time step δ_k and scaling factor M_k as decision variables optimized by classical methods rather than using the fixed hyperparameters of standard FALQON. It reports a comprehensive empirical comparison on all 94 non-isomorphic 3-regular graphs with 12 vertices, claiming statistically significant gains in success probability, evaluation efficiency, and depth-normalized cost versus standard FALQON and several QAOA variants. It further shows that parameters obtained from Optimal FALQON provide superior warm-start initialization for QAOA relative to fixed initialization.

Significance. If the empirical gains survive a full accounting of classical optimization overhead, the work could improve the layer efficiency of feedback-based quantum optimization on NISQ hardware. The exhaustive benchmark over the complete set of 12-vertex 3-regular graphs is a clear strength, enabling definitive within-class comparisons. The QAOA warm-start result is a useful byproduct. Broader significance is constrained by the small instance size and the absence of scaling data or net-cost analysis.

major comments (3)
  1. [§3] §3 (Optimal FALQON formulation): the classical optimizer used to tune δ_k and M_k per layer necessarily incurs multiple cost-function evaluations; the manuscript provides no count of total quantum circuit calls (including optimizer iterations) and therefore cannot substantiate the abstract claim of improved evaluation efficiency relative to standard FALQON's single evaluation per layer.
  2. [§4] §4 (empirical study): all reported results are confined to 12-vertex graphs; because the central efficiency and generalization claims rest on the assumption that classical tuning overhead remains modest at larger sizes, the manuscript must either demonstrate scaling behavior or explicitly bound the regime in which the reported gains are expected to hold.
  3. [§4.3] §4.3 (statistical claims): the abstract asserts 'statistically significant' improvements, yet the text does not specify the exact hypothesis test, correction for multiple comparisons, or effect-size reporting used to support this statement; without these details the strength of the empirical evidence cannot be evaluated.
minor comments (2)
  1. [§2] The definition and normalization procedure for 'depth-normalized cost' should be stated explicitly in §2 or §3 rather than introduced only in the results tables.
  2. [Figures 2-4] Figure captions and axis labels for the success-probability and efficiency plots should include the exact number of independent runs and random seeds used.

Simulated Author's Rebuttal

3 responses · 0 unresolved

We thank the referee for the thorough and constructive review of our manuscript. We address each major comment in detail below and indicate the revisions we plan to make.

read point-by-point responses
  1. Referee: §3 (Optimal FALQON formulation): the classical optimizer used to tune δ_k and M_k per layer necessarily incurs multiple cost-function evaluations; the manuscript provides no count of total quantum circuit calls (including optimizer iterations) and therefore cannot substantiate the abstract claim of improved evaluation efficiency relative to standard FALQON's single evaluation per layer.

    Authors: We agree with the referee that the total quantum circuit calls, including those from the classical optimizer's iterations, were not quantified in the original manuscript. This is an important point for a fair efficiency comparison. In the revised manuscript, we will add a section or subsection detailing the number of quantum circuit evaluations required by the classical optimization procedure for tuning δ_k and M_k. We will report the average and maximum number of cost function evaluations across the benchmarks and use this to substantiate or qualify the claims of improved evaluation efficiency. Additionally, we will clarify that 'evaluation efficiency' refers to the quantum resources needed to reach a target success probability. revision: yes

  2. Referee: §4 (empirical study): all reported results are confined to 12-vertex graphs; because the central efficiency and generalization claims rest on the assumption that classical tuning overhead remains modest at larger sizes, the manuscript must either demonstrate scaling behavior or explicitly bound the regime in which the reported gains are expected to hold.

    Authors: We acknowledge the limitation of our study to 12-vertex graphs, which was chosen to enable an exhaustive comparison over all non-isomorphic instances. While we cannot provide new scaling experiments in this revision, we will explicitly bound the regime by discussing the expected growth of the classical optimization overhead. Specifically, we will note that for graphs where the optimal number of layers remains small (as observed in our results), the overhead is modest, and provide a rough estimate based on the dimensionality of the parameter space. We will also emphasize that the primary contribution is the within-class comparison for this size and flag scaling as future work. revision: partial

  3. Referee: §4.3 (statistical claims): the abstract asserts 'statistically significant' improvements, yet the text does not specify the exact hypothesis test, correction for multiple comparisons, or effect-size reporting used to support this statement; without these details the strength of the empirical evidence cannot be evaluated.

    Authors: We thank the referee for highlighting this omission. In the revised manuscript, we will provide the missing statistical details. We will specify the exact hypothesis test(s) used, any corrections applied for multiple comparisons, and include effect-size reporting to support the statistical significance claims. revision: yes

Circularity Check

0 steps flagged

No significant circularity in derivation chain

full rationale

The paper proposes Optimal FALQON by treating per-layer δ_k and M_k as classically optimizable decision variables, then reports empirical performance gains versus standard FALQON and QAOA on a fixed set of 94 graphs. No derivation step equates a claimed result to its own inputs by construction, no fitted parameter is relabeled as a prediction, and no load-bearing premise reduces to a self-citation chain. The central claims are measured outcomes of an algorithmic variant, not tautological reductions from the quantum circuit equations themselves.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on the empirical performance of classically optimized layer parameters within the existing FALQON and QAOA frameworks; no new physical entities or ad-hoc axioms are introduced beyond standard assumptions of the quantum circuit model.

axioms (1)
  • domain assumption Standard quantum circuit model and NISQ noise assumptions hold for the tested circuit depths
    The method assumes the underlying quantum hardware behaves according to the usual circuit model used in FALQON and QAOA.

pith-pipeline@v0.9.0 · 5460 in / 1288 out tokens · 55381 ms · 2026-05-12T01:03:52.864111+00:00 · methodology

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Reference graph

Works this paper leans on

29 extracted references · 29 canonical work pages · 2 internal anchors

  1. [1]

    A variational eigenvalue solver on a photonic quantum processor,

    A. Peruzzo, J. McClean, P. Shadbolt, M.-H. Yung, X.-Q. Zhou, P. J. Love, A. Aspuru-Guzik, and J. L. O’Brien, “A variational eigenvalue solver on a photonic quantum processor,”Nature Communications, vol. 5, p. 4213, 2014. [Online]. Available: https://doi.org/10.1038/ ncomms5213

  2. [2]

    The theory of variational hybrid quantum-classical algorithms,

    J. R. McClean, J. Romero, R. Babbush, and A. Aspuru-Guzik, “The theory of variational hybrid quantum-classical algorithms,”New Journal of Physics, vol. 18, p. 023023, 2016. [Online]. Available: https://doi.org/10.1088/1367-2630/18/2/023023

  3. [3]

    A Quantum Approximate Optimization Algorithm

    E. Farhi, J. Goldstone, and S. Gutmann, “A quantum approximate optimization algorithm,”arXiv preprint arXiv:1411.4028, 2014. [Online]. Available: https://arxiv.org/abs/1411.4028

  4. [4]

    Feedback-based quantum optimization,

    A. B. Magann, K. M. Rudinger, M. D. Grace, and M. Sarovar, “Feedback-based quantum optimization,”Physical Review Letters, vol. 129, p. 250502, 2022. [Online]. Available: https://doi.org/10.1103/ PhysRevLett.129.250502

  5. [5]

    Stochastic properties of the frequency dynamics in real and synthetic power grids,

    D. Arai, K. N. Okada, Y . Nakano, K. Mitarai, and K. Fujii, “Scalable circuit depth reduction in feedback-based quantum optimization with a quadratic approximation,”Physical Review Research, vol. 7, p. 013035, Jan 2025. [Online]. Available: https://doi.org/10.1103/PhysRevResearch. 7.013035

  6. [6]

    Arute et al., Quantum supremacy using a programmable superconducting processor, Nature 574, 505 (2019), doi:10.1038/s41586-019-1666-5

    F. Arute, K. Arya, R. Babbushet al., “Quantum supremacy using a programmable superconducting processor,”Nature, vol. 574, no. 7779, pp. 505–510, 2019. [Online]. Available: https: //doi.org/10.1038/s41586-019-1666-5

  7. [7]

    Superconducting qubits: Current state of play,

    M. Kjaergaard, M. E. Schwartz, J. Braum ¨uller, P. Krantz, J. I.- J. Wang, S. Gustavsson, and W. D. Oliver, “Superconducting qubits: Current state of play,”Annual Review of Condensed Matter Physics, vol. 11, no. 1, pp. 369–395, 2020. [Online]. Available: https://doi.org/10.1146/annurev-conmatphys-031119-050605

  8. [8]

    Ibm quantum services,

    IBM Research, “Ibm quantum services,” https://www.ibm.com/quantum, 2025, accessed: January 24, 2026

  9. [9]

    Amazon braket pricing,

    Amazon Web Services, “Amazon braket pricing,” https://aws.amazon. com/braket/pricing/, 2026, accessed: January 24, 2026

  10. [10]

    Accelerating feedback-based quantum algorithms through time rescaling,

    L. A. M. Rattighieri, G. E. L. Pexe, B. L. Bernardo, and F. F. Fanchini, “Accelerating feedback-based quantum algorithms through time rescaling,”Physical Review A, vol. 112, p. 042607, 2025. [Online]. Available: https://doi.org/10.1103/qc91-5mj2

  11. [11]

    Robust feedback-based quantum optimization: analysis of coherent control errors,

    M. Legnini and J. Berberich, “Robust feedback-based quantum optimization: analysis of coherent control errors,” in2025 IEEE International Conference on Quantum Control, Computing and Learning (qCCL), 2025, pp. 17–22. [Online]. Available: https: //doi.org/10.1109/qCCL65142.2025.11158422

  12. [12]

    PennyLane: Automatic differentiation of hybrid quantum-classical computations

    V . Bergholm, J. Izaac, M. Schuld, C. Gogolin, C. Blank, K. McK- iernan, and N. Killoran, “Pennylane: Automatic differentiation of hy- brid quantum-classical computations,”arXiv preprint arXiv:1811.04968, 2018

  13. [13]

    D. J. Griffiths and D. F. Schroeter,Introduction to Quantum Mechanics, 3rd ed. Cambridge University Press, 2018

  14. [14]

    Low-depth clifford circuits approximately solve maxcut,

    M. H. M. noz Arias, S. Kourtis, and A. Blais, “Low-depth clifford circuits approximately solve maxcut,”Physical Review Research, vol. 6, p. 023294, 2024. [Online]. Available: https: //doi.org/10.1103/PhysRevResearch.6.023294

  15. [15]

    Multi-angle quantum approximate optimization algorithm,

    R. Herrman, P. C. Lotshaw, J. Ostrowski, T. S. Humble, and G. Siopsis, “Multi-angle quantum approximate optimization algorithm,” Scientific Reports, vol. 12, p. 6781, 2022. [Online]. Available: https://doi.org/10.1038/s41598-022-10555-8

  16. [16]

    The Sage Developers,SageMath, the Sage Mathematics Software System (Version 9.5), 2022,https://www.sagemath.org

  17. [17]

    Practical graph isomorphism,

    B. D. McKay, “Practical graph isomorphism,”Congressus Numerantium, vol. 30, pp. 45–87, 1981, version 2.7: https://pallini.di.uniroma1.it/

  18. [18]

    An efficient method for finding the minimum of a function of several variables without calculating derivatives,

    M. J. D. Powell, “An efficient method for finding the minimum of a function of several variables without calculating derivatives,”The Computer Journal, vol. 7, no. 2, pp. 155–162, 1964

  19. [19]

    A comparison of various classical optimizers for a variational quantum linear solver,

    M. A. Alam, S. Ghosh, T. S. Humble, and N. Imam, “A comparison of various classical optimizers for a variational quantum linear solver,” arXiv preprint arXiv:2106.08682, 2021

  20. [20]

    Warm-starting quantum optimization,

    D. J. Egger, J. Mare ˇcek, and S. Woerner, “Warm-starting quantum optimization,”Quantum, vol. 5, p. 479, jun 2021. [Online]. Available: https://doi.org/10.22331/q-2021-06-17-479

  21. [21]

    Quantum annealing initialization of the quantum approximate optimization algorithm,

    S. H. Sack and M. Serbyn, “Quantum annealing initialization of the quantum approximate optimization algorithm,”Quantum, vol. 5, p. 491, jul 2021. [Online]. Available: https://doi.org/10.22331/ q-2021-07-01-491

  22. [22]

    Lyapunov control-inspired strategies for quantum combinatorial optimization,

    A. B. Magann, K. M. Rudinger, M. D. Grace, and M. Sarovar, “Lyapunov control-inspired strategies for quantum combinatorial optimization,”Physical Review A, vol. 106, p. 062414, 2022. [Online]. Available: https://doi.org/10.1103/PhysRevA.106.062414

  23. [23]

    Lyapunov-based control of quantum systems,

    S. Grivopoulos and B. Bamieh, “Lyapunov-based control of quantum systems,” inProceedings of the 42nd IEEE Conference on Decision and Control, vol. 1. Maui, HI, USA: IEEE, dec 2003, pp. 434–438

  24. [24]

    Individual comparisons by ranking methods,

    F. Wilcoxon, “Individual comparisons by ranking methods,”Biometrics Bulletin, vol. 1, no. 6, pp. 80–83, 1945

  25. [25]

    Hollander, D

    M. Hollander, D. A. Wolfe, and E. Chicken,Nonparametric Statistical Methods, 3rd ed. Wiley, 2013

  26. [26]

    A simple sequentially rejective multiple test procedure,

    S. Holm, “A simple sequentially rejective multiple test procedure,” Scandinavian Journal of Statistics, vol. 6, pp. 65–70, 1979

  27. [27]

    A simplex method for function minimiza- tion,

    J. A. Nelder and R. Mead, “A simplex method for function minimiza- tion,”The Computer Journal, vol. 7, no. 4, pp. 308–313, 1965

  28. [28]

    A direct search optimization method that models the objective and constraint functions by linear interpolation,

    M. J. D. Powell, “A direct search optimization method that models the objective and constraint functions by linear interpolation,” inAdvances in Optimization and Numerical Analysis. Springer, 1994, pp. 51–67

  29. [29]

    The Scipy community,Scipy Lecture Notes, https: //scipy-lectures.org/advanced/mathematical optimization/, 2023, https://scipy-lectures.org/