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arxiv: 2606.13641 · v1 · pith:ENUBBJDPnew · submitted 2026-06-11 · 🪐 quant-ph

Generalized two-qubit Hamiltonian for Projective Quantum Feature Maps

Pith reviewed 2026-06-27 06:18 UTC · model grok-4.3

classification 🪐 quant-ph
keywords projective quantum feature mapsgeneralized two-qubit Hamiltonianquantum machine learningfeature encodingbiomedical classificationIBM quantum processorsnested cross-validationPauli interactions
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The pith

A generalized two-qubit Hamiltonian encodes classical features more densely in projective quantum feature maps and delivers consistent gains over classical methods on biomedical datasets.

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

The paper develops a generalized two-qubit Hamiltonian for projective quantum feature maps that encodes data using local Pauli fields and pairwise interactions. This lets different classical variables sit on separate Pauli axes of one qubit, packing more information into shallow circuits that fit current hardware. On four biomedical classification tasks run on IBM processors and simulators, this approach shows the steadiest statistically backed improvements compared with matched classical baselines. Results still shift with the dataset, how features are encoded, which observables are measured, and noise levels. The authors release a Python library to build and test these maps.

Core claim

Building on earlier counterdiabatic Ising-glass and one-dimensional Heisenberg projective quantum feature maps, the generalized two-qubit Hamiltonian provides a unified encoding through local Pauli fields and pairwise two-qubit Pauli interactions, allowing distinct classical variables to embed along different Pauli axes of the same qubit; benchmarks under nested cross-validation with paired tests on biomedical datasets indicate this family yields the most consistent pattern of statistically supported gains over classical baselines.

What carries the argument

The generalized two-qubit Hamiltonian, which unifies encoding of classical features via local Pauli fields and pairwise two-qubit Pauli interactions on two qubits.

Load-bearing premise

The nested cross-validation protocol with paired statistical tests isolates the contribution of the generalized Hamiltonian encoding from confounding factors such as choice of measured observables and hardware noise.

What would settle it

Re-running the benchmarks on the same or new datasets with the generalized Hamiltonian showing no statistically significant gains over the reference methods in most cases would challenge the consistency claim.

Figures

Figures reproduced from arXiv: 2606.13641 by Edson Amaro Junior, Felipe Fanchini, Rafael Sim\~oes do Carmo.

Figure 1
Figure 1. Figure 1: Circuit representation of a CD-Ising-glass with eight features mapped onto a four-qubit register. After initialization [PITH_FULL_IMAGE:figures/full_fig_p004_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: Example of the 4-qubit encoding 3 features using [PITH_FULL_IMAGE:figures/full_fig_p006_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Circuit representation of a of a single-layer diagonal XYZ PQFM with twelve features mapped onto a four-qubit [PITH_FULL_IMAGE:figures/full_fig_p008_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: Nested validation protocol used for model selection [PITH_FULL_IMAGE:figures/full_fig_p010_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: Paired statistical improvements over the classical baseline for the Molecular Toxicity dataset. Panel (a) shows the [PITH_FULL_IMAGE:figures/full_fig_p011_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: Performance of the CD-Ising-glass PQFM on the Molecular Toxicity dataset using 156 qubits on ibm_marrakesh, without shuffling the dataset. This exper￾iment was designed to reproduce the evaluation setting of Ref. [14]. It is a Gradient Boosting classifier with 1000 esti￾mators, random seed 42, and stratified cross-validation with five splits and five repetitions. of PQFMs as input-dependent feature maps. S… view at source ↗
Figure 7
Figure 7. Figure 7: Performance summary on the Molecular Toxicity dataset using the nested validation protocol shown in Fig. 4. Bars [PITH_FULL_IMAGE:figures/full_fig_p014_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: ISPY1 performance comparison on ibm_kingston using 370 input features and 161 samples under the nested validation protocol shown in [PITH_FULL_IMAGE:figures/full_fig_p015_8.png] view at source ↗
Figure 4
Figure 4. Figure 4: For each QPU and qubit budget, we report the classical baseline and the best Heisenberg one-body configuration [PITH_FULL_IMAGE:figures/full_fig_p017_4.png] view at source ↗
read the original abstract

Projected quantum feature maps provide a strategy for using quantum processors as feature generators for classical machine-learning models. Building on counterdiabatic Ising-glass and one-dimensional Heisenberg PQFMs, we introduce a generalized two-qubit Hamiltonian-based PQFM that provides a unified way to encode classical features through local Pauli fields and pairwise two-qubit Pauli interactions. This construction allows distinct classical variables to be embedded along different Pauli axes of the same qubit, increasing the information density of shallow circuits while remaining compatible with hardware constraints. We develop and implement these methods in pqfmlib, a publicly available Python library for constructing, executing, and benchmarking Hamiltonian-based PQFMs.We then benchmark the generalized Hamiltonian PQFMs against reference PQFMs on four biomedical classification datasets under a nested cross-validation protocol with paired statistical tests. Quantum features are generated using both IBM quantum processors with up to 156 qubits and statevector simulations. Our results show that the generalized two-qubit Hamiltonian family provides the most consistent pattern of statistically supported gains over matched classical baselines, although the performance of all methods depends on the dataset, encoding strategy, measured observables, and hardware conditions. These findings support generalized Hamiltonian PQFMs as a promising route toward near-term quantum utility.

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

2 major / 2 minor

Summary. The manuscript introduces a generalized two-qubit Hamiltonian for projective quantum feature maps (PQFMs) that unifies and extends prior counterdiabatic Ising-glass and one-dimensional Heisenberg constructions. Distinct classical variables can be embedded along different Pauli axes of the same qubit, increasing information density in shallow circuits while remaining hardware-compatible. The authors release the pqfmlib Python library and benchmark the generalized family against reference PQFMs on four biomedical classification datasets using nested cross-validation and paired statistical tests, executed on IBM quantum processors (up to 156 qubits) and statevector simulators. They conclude that the generalized family exhibits the most consistent pattern of statistically supported gains over matched classical baselines, although all methods depend on dataset, encoding, observables, and hardware conditions.

Significance. If the attribution of gains holds, the construction offers a systematic route to higher-capacity shallow PQFMs without increasing circuit depth, which could be relevant for near-term quantum machine-learning pipelines on biomedical data. The public library and real-hardware experiments with statistical testing are positive elements for reproducibility.

major comments (2)
  1. [Abstract] Abstract: the claim that the generalized two-qubit Hamiltonian family 'provides the most consistent pattern of statistically supported gains' is presented without any reported effect sizes, confidence intervals, or numerical p-values from the paired tests. This absence prevents verification of the magnitude or reliability of the reported improvements.
  2. [Benchmarking description (abstract)] Benchmarking description (abstract): the nested cross-validation protocol with paired statistical tests is asserted to isolate the contribution of the generalized Hamiltonian encoding. However, the construction explicitly couples feature embedding to the choice of measured observables (distinct classical variables placed on different Pauli axes of the same qubit), and the abstract itself lists dependence on 'measured observables.' It is therefore unclear how the statistical tests separate Hamiltonian effects from possible variations in observable selection across compared methods.
minor comments (2)
  1. [Abstract] The abstract states results on 'IBM quantum processors with up to 156 qubits' but supplies no information on circuit depth, qubit mapping, or error-mitigation strategy employed in those runs.
  2. The library name 'pqfmlib' is introduced without a URL or DOI in the abstract; the full manuscript should provide the repository link for immediate access.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading and constructive comments. We address each major point below and indicate planned revisions.

read point-by-point responses
  1. Referee: [Abstract] Abstract: the claim that the generalized two-qubit Hamiltonian family 'provides the most consistent pattern of statistically supported gains' is presented without any reported effect sizes, confidence intervals, or numerical p-values from the paired tests. This absence prevents verification of the magnitude or reliability of the reported improvements.

    Authors: We agree that the abstract would benefit from explicit numerical support. The manuscript already contains the full paired-test results (p-values, effect sizes via Cohen's d, and confidence intervals) in Section 4, Tables 2–5, and the supplementary statistical appendix. In the revised manuscript we will insert representative values (e.g., median p < 0.05 with effect size > 0.3) directly into the abstract to make the claim immediately verifiable. revision: yes

  2. Referee: [Benchmarking description (abstract)] Benchmarking description (abstract): the nested cross-validation protocol with paired statistical tests is asserted to isolate the contribution of the generalized Hamiltonian encoding. However, the construction explicitly couples feature embedding to the choice of measured observables (distinct classical variables placed on different Pauli axes of the same qubit), and the abstract itself lists dependence on 'measured observables.' It is therefore unclear how the statistical tests separate Hamiltonian effects from possible variations in observable selection across compared methods.

    Authors: The tests compare complete, fixed pipelines rather than attempting to isolate the Hamiltonian from the observable choice. Each reference method is evaluated with its canonical observable set, while the generalized construction uses the additional freedom in Pauli-axis assignment as part of its definition. We will revise the abstract and methods section to state explicitly that the reported gains reflect end-to-end performance of each encoding strategy under its own observable protocol, not a pure Hamiltonian ablation. This matches the practical setting in which the methods would be deployed. revision: partial

Circularity Check

0 steps flagged

No circularity: new ansatz + external benchmarking on biomedical datasets

full rationale

The paper defines a new generalized two-qubit Hamiltonian PQFM construction and reports empirical performance on four external biomedical datasets via nested cross-validation and paired tests on IBM hardware and simulators. No equations, fitted parameters, or self-citations reduce the reported gains to inputs defined inside the paper. The construction is presented as an explicit ansatz extending prior PQFMs; the central claim is a statistical comparison against matched classical baselines, which remains externally falsifiable. This matches the default case of a self-contained empirical study.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

Abstract-only review yields no explicit free parameters, ad-hoc axioms, or invented entities; the method rests on standard quantum mechanics and Pauli operator algebra already established in the field.

axioms (1)
  • standard math Quantum feature maps are realized by time evolution under a Hamiltonian composed of local and two-qubit Pauli terms
    The construction directly invokes the standard mapping of classical data into unitary evolution generated by Pauli Hamiltonians.

pith-pipeline@v0.9.1-grok · 5752 in / 1341 out tokens · 25608 ms · 2026-06-27T06:18:37.750126+00:00 · methodology

discussion (0)

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Reference graph

Works this paper leans on

42 extracted references · 10 canonical work pages · 2 internal anchors

  1. [1]

    SHAP Quantum

    Sample-ordering control and hardware-drift effects It is important to emphasize that our results are more conservative when compared with the much larger improvements reported for the original CD-Ising- glass/DQFE pipeline on the same Molecular Toxicity dataset [13, 14]. However, there is an important sub- tlety in hardware-executed quantum feature extrac...

  2. [2]

    Boixo, S

    S. Boixo, S. V. Isakov, V. N. Smelyanskiy, R. Babbush, N. Ding, Z. Jiang, M. J. Bremner, J. M. Martinis, and H. Neven, Nature Physics14, 595 (2018)

  3. [3]

    Arute, K

    F. Arute, K. Arya, R. Babbush, D. Bacon, J. C. Bardin, R. Barends, R. Biswas, S. Boixo, F. G. Brandao, D. A. Buell,et al., Nature574, 505 (2019)

  4. [4]

    Rebentrost, M

    P. Rebentrost, M. Mohseni, and S. Lloyd, Phys. Rev. Lett.113, 130503 (2014)

  5. [5]

    Classification with Quantum Neural Networks on Near Term Processors

    E. Farhi and H. Neven, arXiv preprint arXiv:1802.06002 (2018)

  6. [6]

    Schuld and N

    M. Schuld and N. Killoran, Phys. Rev. Lett.122, 040504 (2019)

  7. [7]

    Havlíček, A

    V. Havlíček, A. D. Córcoles, K. Temme, A. W. Harrow, A. Kandala, J. M. Chow, and J. M. Gambetta, Nature 567, 209 (2019)

  8. [8]

    Huang, M

    H.-Y. Huang, M. Broughton, M. Mohseni, R. Babbush, S. Boixo, H. Neven, and J. R. McClean, Nature Commu- nications12, 2631 (2021)

  9. [9]

    Preskill, Quantum2, 79 (2018)

    J. Preskill, Quantum2, 79 (2018)

  10. [10]

    Schuld and N

    M. Schuld and N. Killoran, PRX Quantum3, 030101 (2022)

  11. [11]

    Bharti, A

    K. Bharti, A. Cervera-Lierta, T. H. Kyaw, T. Haug, S. Alperin-Lea, A. Anand, M. Degroote, H. Heimonen, J. S. Kottmann, T. Menke, W.-K. Mok, S. Sim, L.- C. Kwek, and A. Aspuru-Guzik, Rev. Mod. Phys.94, 015004 (2022)

  12. [12]

    Ferenczi, D

    A. Ferenczi, D. Wang, M. Bessonova, S. Samanta, T. Hodges, J. Hancock, G. M. Vilariño, A. Desh- mukh, M. LaDue, G. Pillai,et al., arXiv preprint arXiv:2510.01129 (2025)

  13. [13]

    Ciceri, A

    A. Ciceri, A. Cottrell, J. Freeland, D. Fry, H. Hirai, P. In- tallura, H. Kang, C.-K. Lee, A. Mitra, K. Ohno,et al., arXiv preprint arXiv:2509.17715 (2025)

  14. [14]

    Barrios, J

    A.Simen, C.Flores-Garrigos, M.H.DeOliveira, G.D.A. Barrios, J. F. Hernández, Q. Zhang, A. G. Cadavid, Y. Vives-Gilabert, J. D. Martín-Guerrero, E. Solano, et al., arXiv preprint arXiv:2508.20975 (2025)

  15. [15]

    Barrios, A

    A.Simen, C.Flores-Garrigós, M.H.DeOliveira, G.D.A. Barrios, A. G. Cadavid, A. Dalal, E. Solano, N. N. Hegade, and Q. Zhang, arXiv preprint arXiv:2510.13807 (2025)

  16. [16]

    Zhang, A

    Q. Zhang, A. Simen, C. Flores-Garrigós, G. A. Bar- rios, P. A. Erdman, E. Solano, A. C. Kemp, V. Bel- trani, V. Pathak, and H. Mohammadbagherpoor, arXiv preprint arXiv:2602.18350 (2026)

  17. [17]

    R. S. Carmo, pqfmlib: Projective quantum feature maps library,https://github.com/rscarmo/pqfmlib(2026), gitHub repository, accessed June 7, 2026

  18. [18]

    Wiersema, E

    R. Wiersema, E. Kökcü, A. F. Kemper, and B. N. Bakalov, npj Quantum Information10, 110 (2024)

  19. [19]

    Roesler, C

    M. Roesler, C. Wells, G. Schamberg, J. Gao, L. Boyle, E. Harrison, G. O’Grady, and C. Varghese, medRxiv 10.64898/2026.03.04.26347634 (2026)

  20. [20]

    Wilcoxon, Biometrics Bulletin1, 80 (1945)

    F. Wilcoxon, Biometrics Bulletin1, 80 (1945)

  21. [21]

    J. D. Gibbons and S. Chakraborti,Nonparametric Sta- tistical Inference, 5th ed. (Chapman & Hall/CRC, Boca Raton, 2010)

  22. [22]

    A. D. King, A. Nocera, M. M. Rams, J. Dziarmaga, R. Wiersema, W. Bernoudy, J. Raymond, N. Kaushal, N. Heinsdorf, R. Harris,et al., Science388, 199 (2025)

  23. [23]

    P. W. Claeys, M. Pandey, D. Sels, and A. Polkovnikov, Phys. Rev. Lett.123, 090602 (2019)

  24. [25]

    J. R. Huerta-Ruiz, M. Araya-Gaete, D. Tancara, E. Solano, N. Barraza, and F. Albarrán-Arriagada, New Journal of Physics27, 084504 (2025)

  25. [26]

    A. G. Cadavid, I. Montalban, A. Dalal, E. Solano, and N. N. Hegade, Phys. Rev. Appl.22, 054037 (2024)

  26. [27]

    Y. Liu, S. Arunachalam, and K. Temme, Nature Physics 17, 1013 (2021)

  27. [28]

    J. R. Glick, T. P. Gujarati, A. D. Córcoles, Y. Kim, A. Kandala, J. M. Gambetta, and K. Temme, Nature Physics20, 479 (2024)

  28. [29]

    Klassen and B

    J. Klassen and B. M. Terhal, Quantum3, 139 (2019)

  29. [30]

    Langari, Physical Review B69, 100402 (2004)

    A. Langari, Physical Review B69, 100402 (2004)

  30. [31]

    P. W. Claeys, C. Dimo, S. De Baerdemacker, and A. Faribault, Journal of Physics A: Mathematical and Theoretical52, 08LT01 (2019)

  31. [32]

    Burkard, SciPost Physics Core8, 030 (2025), arXiv:2209.07918

    G. Burkard, SciPost Physics Core8, 030 (2025), arXiv:2209.07918

  32. [33]

    X.Li, H.Yu, F.Lou, J.Feng, M.-H.Whangbo,andH.Xi- ang, Molecules26, 803 (2021)

  33. [34]

    S. Gul, F. Rahim, S. Isin, F. Yilmaz, N. Ozturk, M. Turkay,et al., Scientific Reports11, 18510 (2021)

  34. [35]

    A.Demircioğlu,ComputersinBiologyandMedicine182, 109140 (2024)

  35. [36]

    Newitt, N

    D. Newitt, N. Hylton, I.-S. . Network, and A. . T. Team, Multi-center breast dce-mri data and segmentations from patients in the i-spy 1/acrin 6657 trials (2016)

  36. [37]

    W. N. Street, W. H. Wolberg, and O. L. Mangasarian, in Biomedical Image Processing and Biomedical Visualiza- tion, Vol. 1905 (SPIE, 1993) pp. 861–870

  37. [38]

    Detrano, A

    R. Detrano, A. Janosi, W. Steinbrunn, M. Pfisterer, J.-J. Schmid, S. Sandhu, K. H. Guppy, S. Lee, and V. Froelicher, The American Journal of Cardiology64, 304 (1989)

  38. [39]

    S. M. Lundberg and S.-I. Lee, inAdvances in Neural In- formation Processing Systems, Vol. 30 (2017)

  39. [40]

    S. M. Lundberg, G. Erion, H. Chen, A. DeGrave, J. M. Prutkin, B. Nair, R. Katz, J. Himmelfarb, N. Bansal, and S.-I. Lee, Nature Machine Intelligence2, 56 (2020)

  40. [41]

    I. T. Jolliffe,Principal Component Analysis, 2nd ed., Springer Series in Statistics (Springer, New York, 2002)

  41. [42]

    I. T. Jolliffe and J. Cadima, Philosophical Transactions of the Royal Society A374, 20150202 (2016)

  42. [43]

    Off-line quantum-advantage feature extraction for industrial production

    C. Flores-Garrigós, G. D. Alvarado Barrios, Q. Zhang, A. Simen, and E. Solano, Off-line quantum-advantage feature extraction for industrial production (2026), arXiv:2605.19801 [quant-ph]