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arxiv: 2604.01050 · v2 · submitted 2026-04-01 · 🪐 quant-ph · physics.comp-ph

Recognition: 2 theorem links

· Lean Theorem

Simulated Bifurcation Quantum Annealing

Authors on Pith no claims yet

Pith reviewed 2026-05-13 22:00 UTC · model grok-4.3

classification 🪐 quant-ph physics.comp-ph
keywords simulated bifurcationquantum annealinginter-replica interactionsenergy landscapesoptimization heuristicsbenchmarkingquantum-inspired algorithms
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The pith

Simulated Bifurcation Quantum Annealing adds inter-replica interactions to mimic quantum tunneling and improve results on sparse rugged landscapes.

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

The paper introduces Simulated Bifurcation Quantum Annealing as an extension of simulated bifurcation that incorporates inter-replica interactions. These interactions are meant to emulate quantum tunneling effects while preserving the original method's efficiency and parallelism. The work derives the corresponding equations of motion, examines parameter dependence, and supplies a lightweight auto-tuning procedure. Benchmarking on large-scale instances and smaller problems relevant to current hardware shows consistent gains precisely where standard simulated bifurcation is known to falter. The method remains competitive across a broader range of problem families.

Core claim

SBQA extends simulated bifurcation by adding inter-replica interactions that mimic quantum tunneling. The resulting dynamics retain the computational efficiency and parallelism of the base algorithm yet deliver systematic performance gains on sparse and rugged energy landscapes. Parameter dependence is analyzed and a lightweight auto-tuning strategy is proposed. Comprehensive tests on both large instances and smaller problems show that the approach improves on simulated bifurcation in the regimes where the latter struggles while staying competitive and versatile on the full set of evaluated families.

What carries the argument

Inter-replica interactions incorporated into the simulated bifurcation equations to emulate quantum tunneling.

If this is right

  • SBQA supplies a stronger classical baseline for benchmarking quantum annealers on sparse and rugged instances.
  • The derived equations of motion and auto-tuning procedure lower the barrier to applying the method in practice.
  • The approach extends the reach of bifurcation-based solvers to problem classes previously considered difficult for them.
  • Retained parallelism suggests straightforward scaling on distributed classical hardware.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Hybrid solvers could combine SBQA's classical efficiency with occasional calls to actual quantum hardware on the hardest subproblems.
  • Similar interaction terms might be tested in other classical heuristics to see whether tunneling-like effects can be approximated more broadly.
  • Scaling studies on problem sizes beyond the current benchmarks would clarify whether the observed gains persist at industrial scales.

Load-bearing premise

The performance gains arise specifically because the added interactions reproduce the beneficial effects of quantum tunneling rather than through unrelated mechanisms or tuning artifacts.

What would settle it

A controlled experiment in which SBQA shows no statistically significant improvement over standard simulated bifurcation on the same sparse and rugged test set after comparable parameter tuning would falsify the central performance claim.

Figures

Figures reproduced from arXiv: 2604.01050 by Bart{\l}omiej Gardas, Jakub Paw{\l}owski, Jan Tuziemski, {\L}ukasz Pawela, Pawe{\l} Tarasiuk.

Figure 1
Figure 1. Figure 1: FIG. 1 [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2 [PITH_FULL_IMAGE:figures/full_fig_p005_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3 [PITH_FULL_IMAGE:figures/full_fig_p006_3.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5 [PITH_FULL_IMAGE:figures/full_fig_p007_5.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7 [PITH_FULL_IMAGE:figures/full_fig_p008_7.png] view at source ↗
Figure 9
Figure 9. Figure 9: FIG. 9 [PITH_FULL_IMAGE:figures/full_fig_p009_9.png] view at source ↗
Figure 11
Figure 11. Figure 11: FIG. 11 [PITH_FULL_IMAGE:figures/full_fig_p010_11.png] view at source ↗
Figure 12
Figure 12. Figure 12: FIG. 12 [PITH_FULL_IMAGE:figures/full_fig_p010_12.png] view at source ↗
read the original abstract

We introduce Simulated Bifurcation Quantum Annealing (SBQA), a quantum-inspired optimization algorithm that extends simulated bifurcation by incorporating inter-replica interactions to mimic quantum tunneling. SBQA retains the efficiency and parallelism of simulated bifurcation while improving performance on sparse and rugged energy landscapes. We derive its equations of motion, analyze parameter dependence, and propose a lightweight auto-tuning strategy. A comprehensive benchmarking study on both large-scale problems and smaller instances relevant for current quantum hardware shows that SBQA systematically improves on SBM in the sparse and rugged regimes where SBM is known to struggle, while remaining competitive and versatile across a diverse set of tested problem families. These results position SBQA as a practical quantum-inspired optimization heuristic and a stronger classical baseline for the sparse and rugged regimes studied here.

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 Simulated Bifurcation Quantum Annealing (SBQA) as an extension of simulated bifurcation (SBM) that adds inter-replica interactions to emulate quantum tunneling. It derives the equations of motion, analyzes parameter dependence, proposes a lightweight auto-tuning strategy, and presents benchmarking results claiming systematic performance gains over SBM on sparse and rugged landscapes while remaining competitive on other problem families.

Significance. If the reported gains are shown to arise specifically from the inter-replica mechanism rather than from additional tuning freedom, SBQA would strengthen the set of practical quantum-inspired heuristics and provide a more robust classical baseline for sparse/rugged instances relevant to near-term quantum hardware. The auto-tuning component adds immediate engineering value.

major comments (3)
  1. [Benchmarking study] Benchmarking study (abstract and associated results section): the claim of systematic improvement on sparse/rugged regimes lacks reported error bars, explicit data-split protocols, and confirmation that identical tuning effort was applied to the SBM baseline; without these, it is impossible to determine whether the advantage exceeds what parameter optimization alone would produce.
  2. [Derivation of equations of motion] Equations of motion and inter-replica term (derivation section): no ablation is presented that zeros the inter-replica coupling while retaining the auto-tuner, nor is a non-tunneling perturbation (e.g., random classical coupling of equal strength) compared; this leaves open whether performance gains are mechanistically tied to tunneling emulation or simply to extra degrees of freedom.
  3. [Parameter dependence and auto-tuning] Parameter-dependence analysis: the lightweight auto-tuning strategy is introduced without a quantitative demonstration that the same strategy, when applied to plain SBM, fails to close the reported gap; this directly affects the central mechanistic claim.
minor comments (2)
  1. [Notation] Notation for replica indices and coupling strengths is introduced without a consolidated table; a single reference table would improve readability.
  2. [Abstract] The abstract states that SBQA 'remains competitive across a diverse set of tested problem families' but does not list the families or cite the corresponding tables/figures; explicit cross-references are needed.

Simulated Author's Rebuttal

3 responses · 0 unresolved

We thank the referee for the detailed and constructive report. We have revised the manuscript to incorporate error bars, explicit protocols, additional ablations, and quantitative comparisons of the auto-tuning strategy. Our point-by-point responses follow.

read point-by-point responses
  1. Referee: Benchmarking study (abstract and associated results section): the claim of systematic improvement on sparse/rugged regimes lacks reported error bars, explicit data-split protocols, and confirmation that identical tuning effort was applied to the SBM baseline; without these, it is impossible to determine whether the advantage exceeds what parameter optimization alone would produce.

    Authors: We agree that these statistical and methodological details are necessary for robust claims. In the revised manuscript we now report error bars as standard deviations over 20 independent runs per instance with distinct random seeds. We explicitly document the instance-generation protocols (Erdős–Rényi graphs for sparse cases, standard random rugged landscapes) and the train/validation split used for hyper-parameter search. We also confirm that the identical auto-tuning budget (same number of trials and search ranges) was allocated to both SBQA and the SBM baseline; these details have been added to the methods and results sections. revision: yes

  2. Referee: Equations of motion and inter-replica term (derivation section): no ablation is presented that zeros the inter-replica coupling while retaining the auto-tuner, nor is a non-tunneling perturbation (e.g., random classical coupling of equal strength) compared; this leaves open whether performance gains are mechanistically tied to tunneling emulation or simply to extra degrees of freedom.

    Authors: We acknowledge the value of explicit ablations. The revised derivation section now includes a direct comparison of SBQA against (i) the inter-replica term set to zero while retaining the auto-tuner (recovering auto-tuned SBM) and (ii) a control variant that replaces the tunneling-emulating coupling with random classical inter-replica terms of matched magnitude. The random-coupling control does not reproduce the performance gains, consistent with the specific form of the interaction derived from the quantum-inspired model. We have added a short theoretical paragraph explaining why the chosen inter-replica term corresponds to tunneling emulation rather than generic extra degrees of freedom. revision: yes

  3. Referee: Parameter-dependence analysis: the lightweight auto-tuning strategy is introduced without a quantitative demonstration that the same strategy, when applied to plain SBM, fails to close the reported gap; this directly affects the central mechanistic claim.

    Authors: We have performed the requested control experiments and included them in the revised results. Applying the identical lightweight auto-tuning procedure to standard SBM improves its performance relative to untuned SBM, yet a statistically significant gap remains versus SBQA on the sparse/rugged test sets. These new quantitative comparisons, together with expanded parameter-sensitivity plots for both algorithms, are now presented in the parameter-dependence subsection and support the mechanistic contribution of the inter-replica interactions beyond tuning alone. revision: yes

Circularity Check

0 steps flagged

No significant circularity in derivation chain

full rationale

The paper derives SBQA equations of motion by extending the known SBM dynamics with an added inter-replica coupling term, analyzes parameter dependence, and introduces an auto-tuning heuristic. These steps are presented as explicit constructions rather than reductions to fitted outputs. Performance claims rest on external benchmarking across problem families rather than any quantity being redefined or predicted from the same fitted parameters used in the derivation. No self-citation load-bearing steps, uniqueness theorems, or ansatz smuggling appear in the provided text. The derivation remains self-contained against the SBM baseline and the stated benchmarking protocol.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Only the abstract is available; no explicit free parameters, axioms, or invented entities can be extracted beyond the high-level description of inter-replica interactions.

pith-pipeline@v0.9.0 · 5445 in / 1005 out tokens · 19857 ms · 2026-05-13T22:00:40.871338+00:00 · methodology

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Reference graph

Works this paper leans on

57 extracted references · 57 canonical work pages · 2 internal anchors

  1. [1]

    Restricted connectivity leads to the necessity of embedding [45], which in turn significantly degrades performance and limits the size of instances that can be studied

    Large-scale Zephyr instances One of the major challenges for quantum hardware is the structure of couplings between individual qubits (physical or logical), which defines the so-called working graph of the device. Restricted connectivity leads to the necessity of embedding [45], which in turn significantly degrades performance and limits the size of insta...

  2. [2]

    A promising approach, called Quantum Annealing Correction (QAC), was put forth in Ref

    Large-scale Quantum Annealing Correction (QAC) problems It is likely that genuine quantum advantage on near- term quantum annealers, if possible, will require some form of error correction. A promising approach, called Quantum Annealing Correction (QAC), was put forth in Ref. [46], and recently used in an attempt to demon- strate quantum scaling advantage...

  3. [3]

    2D and 3D tile planting In the context of TTεstudies, it is desirable to have access to instances spanning a wide range of sizes and hardness, with known ground state energies, to avoid the pitfalls of extrapolating from small sizes and relying on suboptimal reference energies. We thus turn our atten- tion to the so-called planted solution instances, whic...

  4. [4]

    3D spin glasses on D-Wave quantum annealer We start with benchmarks on 3D spin glasses, with couplings distributed according to the standard normal distribution. This is a modification of the instances al- ready studied in the context of combinatorial optimiza- tion and quantum annealing, for which both the D-Wave annealer and DTSQA performed very well [2...

  5. [5]

    easy” targets and second column to “hard

    Higher-order binary optimization on heavy-hex topology For our final set of benchmarks, we consider a dif- ferent class of problems, namely higher-order binary optimization (HUBO) problems constructed from the heavy-hexagon topology of IBM quantum processors [48]. These problems have recently emerged as a challeng- ing benchmark set for optimization routi...

  6. [6]

    J. M. Weinand, K. S¨ orensen, P. San Segundo, M. Kleine- brahm, and R. McKenna, Research trends in combinato- rial optimization, Int. Trans. Oper. Res.29, 667 (2022)

  7. [7]

    M. S. Martins, J. M. Sousa, and S. Vieira, A systematic review on reinforcement learning for industrial combina- torial optimization problems, Applied Sciences15, 1211 (2025)

  8. [8]

    M. A. Rahman, R. Sokkalingam, M. Othman, K. Biswas, L. Abdullah, and E. Abdul Kadir, Nature-inspired meta- heuristic techniques for combinatorial optimization prob- lems: Overview and recent advances, Mathematics9, 2633 (2021)

  9. [9]

    Mohseni, P

    N. Mohseni, P. L. McMahon, and T. Byrnes, Ising ma- chines as hardware solvers of combinatorial optimization problems, Nat. Rev. Phys.4, 363 (2022)

  10. [10]

    Lucas, Ising formulations of many np problems, Front

    A. Lucas, Ising formulations of many np problems, Front. Phys.2(2014)

  11. [11]

    Yarkoni, E

    S. Yarkoni, E. Raponi, T. B¨ ack, and S. Schmitt, Quan- tum annealing for industry applications: Introduction and review, Rep. Prog. Phys.85, 104001 (2022)

  12. [12]

    L. P. Yulianti and K. Surendro, Implementation of quan- tum annealing: A systematic review, IEEE Access10, 73156 (2022)

  13. [13]

    Abbas, A

    A. Abbas, A. Ambainis, B. Augustino, A. B¨ artschi, and H. Buhrman et al., Challenges and opportunities in quan- tum optimization, Nature Reviews Physics6, 718 (2024)

  14. [14]

    Pelofske, Comparing three generations of d-wave quan- tum annealers for minor embedded combinatorial opti- mization problems, Quantum Sci

    E. Pelofske, Comparing three generations of d-wave quan- tum annealers for minor embedded combinatorial opti- mization problems, Quantum Sci. Technol.10, 025025 (2025)

  15. [15]

    Gomez-Tejedor, E

    A. Gomez-Tejedor, E. Osaba, and E. Villar-Rodriguez, Addressing the minor-embedding problem in quantum annealing and evaluating state-of-the-art algorithm per- formance (2025), arXiv:2504.13376 [quant-ph]

  16. [16]

    A. D. King, S. Suzuki, J. Raymond, A. Zucca, T. Lanting, F. Altomare, A. J. Berkley, S. Ejtemaee, E. Hoskinson, S. Huang,et al., Coherent quantum annealing in a pro- grammable 2,000 qubit ising chain, Nat. Phys.18, 1324 (2022)

  17. [17]

    Pelofske, G

    E. Pelofske, G. Hahn, and H. N. Djidjev, Noise dynamics of quantum annealers: estimating the effective noise us- ing idle qubits, Quantum Sci. Technol.8, 035005 (2023)

  18. [18]

    A. D. King, A. Nocera, M. M. Rams, J. Dziarmaga, R. Wiersema, W. Bernoudy, J. Raymond, N. Kaushal, N. Heinsdorf, R. Harris, K. Boothby, F. Altomare, M. Asad, A. J. Berkley, M. Boschnak,et al., Beyond- classical computation in quantum simulation, Science 388, 199 (2025)

  19. [19]

    Tindall, A

    J. Tindall, A. Mello, M. Fishman, M. Stoudenmire, and D. Sels, Dynamics of disordered quantum systems with two- and three-dimensional tensor networks (2025), arXiv:2503.05693 [quant-ph]

  20. [20]

    Mauron and G

    L. Mauron and G. Carleo, Challenging the quantum ad- vantage frontier with large-scale classical simulations of annealing dynamics (2025), arXiv:2503.08247 [quant-ph]

  21. [21]

    Recent quantum runtime (dis)advantages

    J. Tuziemski, J. Paw lowski, P. Tarasiuk, L. Pawela, and B. Gardas, Recent quantum runtime (dis)advantages (2025), arXiv:2510.06337 [quant-ph]

  22. [22]

    Munoz-Bauza and D

    H. Munoz-Bauza and D. Lidar, Scaling advantage in ap- proximate optimization with quantum annealing, Phys. Rev. Lett.134, 160601 (2025)

  23. [23]

    Pawlowski, P

    J. Pawlowski, P. Tarasiuk, J. Tuziemski, L. Pawela, and B. Gardas, Closing the quantum-classical scaling gap in approximate optimization (2025), arXiv:2505.22514 [quant-ph]

  24. [24]

    M. J. Schuetz, J. K. Brubaker, and H. G. Katzgraber, Combinatorial optimization with physics-inspired graph neural networks, Nat. Mach. Intell.4, 367 (2022)

  25. [25]

    Honari-Latifpour, M

    M. Honari-Latifpour, M. S. Mills, and M.-A. Miri, Com- binatorial optimization with photonics-inspired clock models, Commun. Phys.5, 104 (2022)

  26. [26]

    Zhang, Q

    T. Zhang, Q. Tao, B. Liu, and J. Han, A review of sim- ulation algorithms of classical ising machines for combi- natorial optimization, in2022 IEEE International Sym- posium on Circuits and Systems (ISCAS)(IEEE, 2022) pp. 1877–1881

  27. [27]

    Zeng, X.-P

    Q.-G. Zeng, X.-P. Cui, B. Liu, Y. Wang, and P. Mosharev et al., Performance of quantum annealing inspired algo- rithms for combinatorial optimization problems, Com- munications Physics7, 249 (2024)

  28. [28]

    Goto, Bifurcation-based adiabatic quantum compu- tation with a nonlinear oscillator network, Sci

    H. Goto, Bifurcation-based adiabatic quantum compu- tation with a nonlinear oscillator network, Sci. Rep.6, 21686 (2016)

  29. [29]

    H. Goto, K. Tatsumura, and A. R. Dixon, Combinatorial optimization by simulating adiabatic bifurcations in non- linear hamiltonian systems, Sci. Adv.5, eaav2372 (2019)

  30. [30]

    H. Goto, K. Endo, M. Suzuki, Y. Sakai, and Taro et al., High-performance combinatorial optimization based on classical mechanics, Sci. Adv.7, eabe7953 (2021)

  31. [31]

    Kanao and H

    T. Kanao and H. Goto, Simulated bifurcation for higher- order cost functions, Applied Physics Express16, 014501 (2022)

  32. [32]

    J. Hou, A. Barzegar, and H. G. Katzgraber, Direct com- parison of stochastic driven nonlinear dynamical systems for combinatorial optimization, Phys. Rev. E112(2025)

  33. [33]

    Quantumz.io, VeloxQ QUBO solver (2025), accessed: 2025-01-31

  34. [34]

    Chowdhury, N

    S. Chowdhury, N. A. Aadit, A. Grimaldi, E. Raimondo, A. Raut, P. A. Lott, J. H. Mentink, M. M. Rams, F. Ricci-Tersenghi, M. Chiappini, L. S. Theogarajan, T. Srimani, G. Finocchio, M. Mohseni, and K. Y. Cam- sari, Pushing the boundary of quantum advantage in hard combinatorial optimization with probabilistic com- puters, Nature Communications16(2025)

  35. [35]

    K. Y. Camsari, S. Chowdhury, and S. Datta, Scalable emulation of sign-problem–free hamiltonians with room- temperature p-bits, Phys. Rev. Appl.12(2019)

  36. [36]

    M. Suzuki, Relationship between d-dimensional quan- tal spin systems and (d+1)-dimensional ising systems: Equivalence, critical exponents and systematic approx- imants of the partition function and spin correlations, Prog. Theor. Phys.56, 1454 (1976)

  37. [37]

    VeloxQ: A Fast and Efficient QUBO Solver

    J. Pawlowski, J. Tuziemski, P. Tarasiuk, A. Przy- bysz, R. Adamski, K. Hendzel, L. Pawela, and B. Gar- das, VeloxQ: A fast and efficient QUBO solver (2025), arXiv:2501.19221 [quant-ph]

  38. [38]

    Perera, F

    D. Perera, F. Hamze, J. Raymond, M. Weigel, and H. G. Katzgraber, Computational hardness of spin-glass problems with tile-planted solutions, Phys. Rev. E101, 023316 (2020)

  39. [39]

    Hamze, D

    F. Hamze, D. C. Jacob, A. J. Ochoa, D. Perera, W. Wang, and H. G. Katzgraber, From near to eter- 13 nity: Spin-glass planting, tiling puzzles, and constraint- satisfaction problems, Physical Review E97(2018)

  40. [40]

    A. D. King, J. Raymond, T. Lanting, R. Harris, A. Zucca, F. Altomare, A. J. Berkley, K. Boothby, S. Ejtemaee, C. Enderud, E. Hoskinson, S. Huang, E. Ladizinsky, A. J. R. MacDonald, G. Marsden, R. Molavi, T. Oh, G. Poulin-Lamarre, M. Reis, C. Rich, Y. Sato, N. Tsai, M. Volkmann, J. D. Whittaker, J. Yao, A. W. Sand- vik, and M. H. Amin, Quantum critical dyn...

  41. [41]

    Chandarana, A

    P. Chandarana, A. G. Cadavid, S. V. Romero, A. Simen, E. Solano, and N. N. Hegade, Runtime quantum advantage with digital quantum optimization (2025), arXiv:2505.08663 [quant-ph]

  42. [42]

    Paw lowski, P

    J. Paw lowski, P. Tarasiuk, Tuziemski, L. Pawela, and B. Gardas, Simulated bifurcation quantum annealing - data repository,https://github.com/quantumz-io/ SBQA_benchmarks(2026), GitHub repository

  43. [43]

    See Supplemental Material for a derivation of the Simulated Quantum Annealing Hamiltonian, as well as fine-grained analysis of the benchmarks on hardware- compatible instances

  44. [44]

    Zhang and J

    T. Zhang and J. Han, Quantized simulated bifurcation for the ising model, in2023 IEEE 23rd International Conference on Nanotechnology (NANO)(2023) pp. 715– 720

  45. [45]

    Hamze, J

    F. Hamze, J. Raymond, C. A. Pattison, K. Biswas, and H. G. Katzgraber, The Wishart planted ensemble: A Tunably-Rugged pairwise Ising model with a first- order phase transition, Physical Review E101, 052102 (2020)

  46. [46]

    Tasseff, T

    B. Tasseff, T. Albash, Z. Morrell, M. Vuffray, A. Y. Lokhov, S. Misra, and C. Coffrin, On the emerging po- tential of quantum annealing hardware for combinatorial optimization, J. Heuristics30, 325 (2024)

  47. [47]

    Schulz, D

    S. Schulz, D. Willsch, and K. Michielsen, Learning-driven annealing with adaptive hamiltonian modification for solving large-scale problems on quantum devices, Quan- tum9, 1898 (2025)

  48. [48]

    T. F. Rønnow, Z. Wang, J. Job, S. Boixo, S. V. Isakov, D. Wecker, J. M. Martinis, D. A. Lidar, and M. Troyer, Defining and detecting quantum speedup, Science345, 420–424 (2014)

  49. [49]

    A. A. Gangat, Linear-time classical approximate opti- mization of cubic-lattice classical spin glasses, Physical Review Applied25(2026)

  50. [50]

    D-Wave, Minor embedding, accessed: 2025-01-30

  51. [51]

    K. L. Pudenz, T. Albash, and D. A. Lidar, Error- corrected quantum annealing with hundreds of qubits, Nat. Commun.5, 3243 (2014)

  52. [52]

    Boothby, P

    K. Boothby, P. Bunyk, J. Raymond, and A. Roy, Next-generation topology of d-wave quantum processors (2020), arXiv:2003.00133 [quant-ph]

  53. [53]

    IBM Quantum, The heavy-hex lattice: A new quantum processor topology (2021), accessed: 2026-01-17

  54. [54]

    Tuziemski, J

    J. Tuziemski, J. Paw lowski, P. Tarasiuk, L. Pawela, and B. Gardas, Recent quantum runtime (dis)advantages – code repository,https://github.com/quantumz-io/ quantum-runtime-disadvantage(2025), GitHub reposi- tory

  55. [55]

    S. V. Romero, A.-M. Visuri, A. G. Cadavid, A. Simen, E. Solano, and N. N. Hegade, Bias-field digitized coun- terdiabatic quantum algorithm for higher-order binary optimization, Communications Physics8(2025)

  56. [56]

    D-Wave Systems, Inc.,dimod.make quadratic, Online documentation (Ocean SDK), accessed: 2026-01-15

  57. [57]

    I. G. Rosenberg, Reduction of bivalent maximization to the quadratic case, Cah. Cent. Etud. Rech. Oper.17, 71 (1975). S1 Supplemental Material: Simulated Bifurcation Quantum Annealing In the Supplemental Material we present a concise derivation of the Simulated Quantum Annealing Hamiltonian, as well as fine-grained analysis of the benchmarks on hardware-c...