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REVIEW 3 major objections 5 minor 6 cited by

Explainable AI-assisted Optimization for Feynman Integral Reduction

T0 review · 3 major / 5 minor · reviewed 2026-08-07 · deepseek-v4-flash

Pith's one-line read An AI-designed ordering rule cuts the seed count in Feynman integral reduction by up to a factor of 3,058.

desk verdict Useful and honest, but the headline improvement is not isolated from the category-selection algorithm; needs an ablation before the priority function gets credit. read the letter →

arxiv 2502.09544 v1 pith:IFYWSF36 submitted 2025-02-13 hep-ph hep-th

classification hep-phhep-th
keywords Feynmanintegralsintegration-by-partsreductionLaportaalgorithmpriorityfunctionFunSearchlargelanguagemodelsgeneticalgorithmsphase-space
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

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

The reading

This paper claims that the computationally hard part of Feynman integral evaluation — integration-by-parts (IBP) reduction, which solves large linear systems generated from 'seeding' integrals — can be made much cheaper by sorting the seeds with one explicit formula. The formula is a priority function that ranks each candidate seed by its distance from the origin in index space plus its distance from the target integral; an AI search called FunSearch discovered its shape on the simplest one-loop case, and the authors generalized it by hand to arbitrary numbers of loops and legs. Applied to five-loop six-particle phase-space integral families, the priority function cuts the required number of seeds by up to a factor of 3,058, turning reductions that previously needed more than 400 GB of memory into runs that finish on a laptop in under two minutes. If the transfer holds, IBP reduction stops being the main bottleneck for a wide class of higher-order calculations.

What carries the argument

The load-bearing object is the Ellipse-type priority function $F_0$ of Eq. (16), which assigns each candidate seeding integral a rank equal to minus the sum of two geometric quantities in index space: an $\ell^m$ norm of its propagator indices (a measure of how many dots and numerators it carries) and the Euclidean distance from the seeding point to the target integral. The name records its discovery path: on the one-loop massless bubble problem, FunSearch — a search that evolves short programs through a large language model combined with genetic algorithms — first reproduced the standard Laporta priority (a diagonal line in index space), then a Box priority, then converged to the Ellipse-type form, which the authors read off from the evolved code and generalized to any loop and leg count. Functionally, $F_0$ defines a nested chain of subsets $S_i$ of the seeding set, so the smallest subset sufficient to reduce the target can be located by binary search; the multi-loop applications refine this by sorting seeds into categories and selecting the first $M$ and $G$ categories with a relaxation factor $a = 1/3$.

What would settle it

Run $F_0$ with $m = 2$ on a multi-loop family not used in the paper — say a different non-planar five-loop phase-space family or a six-loop propagator integral with several dotted lines and numerators — and compare the required seed count and peak memory against the best improved-seeding scheme for that family; if the improvement factor collapses toward one, or the solver fails where improved seeding succeeds, the claimed transferability is refuted. A more direct check: evolve a priority function with FunSearch on a genuine two-loop IBP problem; if the best evolved function never beats the Ellipse-type $F_0$ carried over from one loop, the scalability argument loses its evidentiary base.

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Extended reading notes

Core claim

The paper's central claim is that the priority function $F_0$ of Eq. (16), $$F_0(I(n_i); I_{\rm target}(t_i)) = -\left[\left(\sum_i |n_i|^m\right)^{1/m} + \left(\sum_i (n_i - t_i)^2\right)^{1/2}\right],$$ with $m \in \{1,2,4,\infty\}$ and the first term read as $\max_i |n_i|$ for $m = \infty$, is a near-universal way to order IBP seeding integrals: it penalizes seeds that carry dots or numerators (large $\ell^m$ norm) and seeds far from the target integral in index space (large Euclidean distance). Ranked by $F_0$, the seeds generated by conventional schemes arrange into nested subsets, and a binary search locates the smallest subset that still solves the target; memory use is roughly proportional to the size of that subset. On the one-loop problem where the function was evolved, the required subset shrinks by about a factor of five; on the five-loop planar and non-planar families the seed count falls by up to 24.8 times for the hardest reachable top-sector integrals and by 3,058 times (planar) and 1,060 times (non-planar) for sub-sector integrals with many dots and numerators, converting out-of-memory failures into fast laptop-scale reductions.

Load-bearing premise

The load-bearing premise is that the two-dimensional index space of the one-loop massless bubble is representative enough that a priority function optimized there, after human generalization, still works for five-loop six-particle phase-space families with 20 propagators and up to 46 master integrals — a transfer the paper asserts rather than proves, and one its own appendix undercuts slightly by reporting that running FunSearch directly on two-loop problems found nothing better than the Box priority.

Editorial extensions

If this is right

  • The five-loop planar top-sector integrals $s_{10}$ and $s_{12}$, which the improved-seeding baseline cannot complete within 400 GB of memory, become computable, and the planar $d_5$ reduction finishes in under two minutes on a standard laptop.
  • The improvement factor grows with target complexity across the tested range (about 1.0x for the simplest planar top-sector seeds up to 24.8x for $s_{12}$ and 3,058x for $d_5$), so the method pays off most where previous algorithms failed outright.
  • The same hand-generalized priority function works for planar and non-planar integral families, for single-target reductions, and for a 955-target dimensional-recurrence problem in which it halves the seed count relative to improved seeding.
  • Because $F_0$ is a short, interpretable expression rather than a trained black box, it can be ported to new integral families and refined by human experts without rerunning the search.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • If the one-loop-to-five-loop transfer is as general as the paper claims, the same recipe — evolve a priority function on a toy problem with FunSearch, then have an expert generalize the closed form — could be applied to other combinatorial bottlenecks in amplitude computation, such as seed selection for syzygy-based or block-triangular reduction schemes.
  • The paper optimizes seed count rather than solve time, and says so; a priority function tuned directly against equation-solving time could produce further speedups beyond the reported ratios, since the fastest seed set and the smallest seed set need not coincide.
  • The appendix's multi-target variant of Eq. (B1) was only shown to be at least as good as the single-target Ellipse priority; comparing it directly with the recursive single-target strategy on the 955-target problem is a cheap, natural next experiment.
  • Only the $m=2$ variant was used in the multi-loop benchmarks, so the sensitivity of the reported gains to the norm choice ($m=1,4,\infty$) is untested; applying those variants to a hard non-planar family would show whether the improvement is robust to that choice.
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Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

3 major / 5 minor

Summary. The paper proposes a method to reduce the size of integration-by-parts (IBP) systems by ordering seeding integrals with a priority function discovered by the FunSearch algorithm on a one-loop massless bubble integral, then generalized by human experts to the Ellipse-type function F0 in Eq. (16). The authors apply F0, together with a category-based subset-selection algorithm, to planar and non-planar five-loop six-particle phase-space integral families. Tables I and II report large reductions in the number of seeding integrals, up to a factor of 3058 for a planar integral (d5) and 1060 for a non-planar integral (d5), compared to an improved-seeding baseline, and the paper claims these reductions make previously infeasible IBP reductions tractable.

Significance. If the reported reductions are genuinely attributable to the discovered priority function F0, this would be a practically valuable and interpretable heuristic for one of the main computational bottlenecks in multi-loop amplitude calculations. The combination of FunSearch on a simple problem with human transfer to harder problems is a promising methodology, and the target integrals (five-loop, six-particle phase-space, up to 46 master integrals) are nontrivial and of direct interest. The paper's strengths are the explicit, closed-form priority function (Eq. (16)), the use of FiniteFlow for the main comparisons, and the clear statement of the algorithm in Sec. VI. However, as detailed below, the current evidence does not isolate the effect of the priority function from the subset-selection procedure, so the quantitative claims require additional experiments before they can be fully credited.

major comments (3)
  1. [Sec. VI, Tables I and II] The comparison labeled 'Priority function F0' in Tables I and II includes the full category-selection and search algorithm described in Sec. VI (steps 1–5, Eq. (17), with relaxation factor a=1/3), whereas the 'Improved seeding' baseline is the full minimal seeding set without this selection. The paper never runs the same selection algorithm with a different ordering, such as the Laporta priority of Eq. (14), the Box priority of Listing 3, or a random order. Because a complete seeding set contains many redundant equations, a subset-selection procedure can in principle reduce 21,740,796 seeds to 7,109 even with a generic ordering. Thus the reported factors of 3058 (planar d5) and 1060 (non-planar d5) do not currently establish the efficacy of Eq. (16) in isolation; they measure the combined pipeline. Please add an ablation that applies the identical Sec. VI search algorithm with alternative priority functions, including Box and Laporta, for at least the d5 cases in both families.
  2. [Sec. IV–V, Appendix B] The priority function F0 in Eq. (16) is not itself the FunSearch output; it is a human generalization (with m chosen as 2) of an evolved one-loop function. Section IV states 'we hope to obtain a general best-estimated priority function under a simpler IBP problem and naturally extend it', and Appendix B concedes that on two-loop problems FunSearch did not beat Box priority. The multi-loop results therefore depend critically on the human transfer step, and the only direct evidence that Eq. (16) outperforms Box priority is the one-loop factor-of-five improvement in Sec. V (with a single reported target, I(15,10)). To support the central claim that F0 is a 'best-estimated priority function', the authors should compare Eq. (16) against Box priority and Laporta priority on the same multi-loop benchmarks using the same selection protocol.
  3. [General reproducibility (Secs. IV–VI)] No code or data are shipped, and the exact procedure for constructing the categories used in Sec. VI is not specified beyond 'O(10^2) categories are produced for O(10^5) seeding integrals'. The 'improved seeding' minimal pattern search is also not described algorithmically. Timings in Tables I and II are single numerical sample points with no run-to-run variation or detailed machine characterization. For a computational paper whose central contribution is an algorithm, this is insufficient for independent verification. Please provide the implementation, or at least the exact category-generation rules, the optimized seeding vectors, and the binary-search/relaxation details, together with at least a few repeated timing runs for one representative case.
minor comments (5)
  1. [Table I and Table II captions] The notation a/b and a/b/c is explained, but the columns NI/NP and TI/TP are not defined explicitly in the table captions; clarify that these are ratios of seed counts and timings between the F0 column and the improved-seeding column.
  2. [Sec. VI, Eq. (17)] The quantities Ntot and Nm are defined in text, but the relation to the 'first M categories' is ambiguous when multiple sets of M categories could span all master integrals; state whether M is chosen by a deterministic rule and how ties are broken.
  3. [Sec. VI.A, last paragraph] The sentence claiming the d5 reduction 'can now be performed on a standard laptop in under two minutes' appears inconsistent with Table I, which reports 47.7 seconds to learn and 2.24 seconds to solve on a Xeon Gold 6148 with 768 GB RAM; please reconcile or remove the laptop claim.
  4. [Sec. VI.A, after Table I] The text says 'the reduction including the reconstruction of D can now be performed...', but no details of the reconstruction step are given; define D and the reconstruction procedure, or cite the FiniteFlow description.
  5. [Appendix A and Fig. 2 and Fig. 4] Figures 2 and 4 appear to contain garbled or mis-encoded text that is not readable; please regenerate these figures with proper font handling.

Circularity Check

0 steps flagged · score 0.0 of 10

No significant circularity: the priority function is evolved on a one-loop toy problem and tested out-of-sample on multi-loop families; no fitted parameter or self-citation is load-bearing.

full rationale

The paper's derivation chain is self-contained in the sense relevant to circularity. The priority function F0 in Eq. (16) is obtained by running FunSearch on the one-loop massless bubble (Sec. V), with fitness given by the average minimal seeding count for 30 one-loop targets (Appendix A, Eq. (A1)). The multi-loop benchmarks in Sec. VI (planar and non-planar five-loop phase-space families) are not used in the search or in any parameter fit; the generalized form Eq. (16) is transferred to these benchmarks out-of-sample after a human generalization step. No equation in the paper reduces by construction to a fitted parameter, and no result is imported from a self-citation chain: the cited building blocks (Laporta seeding [6], improved seeding [19,72,73], FiniteFlow [31], FunSearch [34]) are external and independently documented. The paper even reports an honest negative result in Appendix B, stating that running FunSearch directly on two-loop problems 'no results surpassing the Box priority were observed,' which is inconsistent with a story in which the reported gains are forced by the algorithm's definition. The main validity concern is an ablation gap: the 3058x and 1060x factors compare F0 plus the category-selection/search algorithm of Sec. VI against the full improved-seeding set, without a control run using Laporta, Box, or random priority under the same selection protocol. That is a benchmarking confound, not circularity, and does not change the circularity score.

Assumptions & free parameters 3 free parameters · 4 assumptions · 0 invented entities

The central claim is an empirical heuristic, so the ledger is dominated by modeling assumptions about representativeness and proportionality rather than fitted physics parameters.

free parameters (3)
  • m, exponent in Eq. (16) = m=2 (chosen from {1,2,4,inf})
    Human-selected after FunSearch runs; changes the norm shape of the priority function and is not fitted to the multi-loop benchmarks.
  • relaxation factor a in Eq. (17) = 1/3
    Set by hand for all examples; no sensitivity scan is reported.
  • improved seeding pattern (g0,g1,...) and dmax for baselines = planar: (0,-1,-1,-2,...), dmax=0; non-planar: (0,-1,-2,-3,...), dmax=1
    Hand-chosen baseline configurations define the 'improved seeding' comparison; the reported improvement factors depend on this choice.
assumptions (4)
  • standard math Integration-by-parts identities in dimensional regularization, Eq. (2), and reverse unitarity, Eq. (3), provide complete recurrence relations for Feynman integrals.
    Standard background for IBP reduction; the paper uses these as the starting point.
  • domain assumption Memory usage and runtime of IBP reduction scale approximately with the number of seeding integrals.
    Sec. IV states this proportionality to justify minimizing the size of the seeding subset; it is an approximation and is not separately validated for the sparse solver used.
  • domain assumption The one-loop massless bubble integral family is representative enough that a priority function optimized there extends to multi-loop, multi-scale planar and non-planar integrals.
    Sec. IV says a general priority function can be obtained under a simpler problem and naturally extended; the paper's multi-loop results depend on this transfer.
  • domain assumption The seed box with side length 10+t1+t2 is large enough that the evolved priority reflects properties of the index space rather than the box boundary.
    Sec. IV makes this assumption to justify transferring the function to other problems; if false, the found priority could be an artifact of the finite search box.

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Cite this review

Pith. "Pith review of Explainable AI-assisted Optimization for Feynman Integral Reduction." pith.science (2026). https://pith.science/paper/IFYWSF36

@misc{pith2026250209544,
  author       = {Pith},
  title        = {Pith review of: Explainable AI-assisted Optimization for Feynman Integral Reduction},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/IFYWSF36}},
  note         = {Machine review of arXiv:2502.09544}
}
read the original abstract

We present a novel approach to optimizing the reduction of Feynman integrals using integration-by-parts identities. By developing a priority function through the FunSearch algorithm, which combines large language models and genetic algorithms, we achieve significant improvements in memory usage and computational efficiency compared to traditional methods. Our approach demonstrates substantial reductions in the required seeding integrals, making previously intractable integrals more manageable. Tested on a variety of Feynman integrals, including one-loop and multi-loop cases with planar and non-planar configurations, our method demonstrates remarkable scalability and adaptability. For reductions of certain Feynman integrals with many dots and numerators, we observed an improvement by a factor of 3058 compared to traditional methods. This work provides a powerful and interpretable framework for optimizing IBP reductions, paving the way for more efficient and practical calculations in high-energy physics.

Figures

Figures reproduced from arXiv: 2502.09544 by the authors.

Figure 1
Figure 1. FIG. 1: This flowchart outlines the operational sequence of the FunSearch algorithm, which is designed to optimize [PITH_FULL_IMAGE:figures/full_fig_p004_1.png] view at source ↗
Figure 2
Figure 2. FIG. 2: Visualization of the Laporta, Box, and Ellipse-like priority. The target integral [PITH_FULL_IMAGE:figures/full_fig_p006_2.png] view at source ↗
Figure 3
Figure 3. FIG. 3: Two six-particle phase-space integral families [PITH_FULL_IMAGE:figures/full_fig_p007_3.png] view at source ↗
Figures from the paper (1 more)
Figure 4
Figure 4. Figure 4: FIG. 4: Evolution of the average seeding integral [PITH_FULL_IMAGE:figures/full_fig_p014_4.png]

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Reference graph

Works this paper leans on

95 extracted references · 12 canonical work pages · cited by 6 Pith papers

  1. [1]

    Count the total number of initial seeding integrals, denoted as Ntot

  2. [2]

    Let the number of seeding inte- grals in these first M categories be Nm

    From left to right, identify the first M categories in which the seeding integrals collectively span all master integrals. Let the number of seeding inte- grals in these first M categories be Nm

  3. [3]

    (17) Identify the first G categories that collectively con- tain at least Nr seeding integrals

    Introduce an adjustable relaxation factor 0 ≤ a ≤ 1 and define Nr = N a tot N 1−a m . (17) Identify the first G categories that collectively con- tain at least Nr seeding integrals

  4. [4]

    Solve the resulting linear equations using the sparse solver provided in FiniteFlow

    Generate IBP equations separately from the seed- ing integrals in the first M and first G categories. Solve the resulting linear equations using the sparse solver provided in FiniteFlow. If both cases suc- cessfully reduce the target integrals, we stop. If only the second case is sufficient, we use all seed- ing integrals for reductions and also apply a b...

  5. [5]

    The above algorithm also improves the search time com- pared to a direct binary search approach

    The final selection of categories directly determines the required seeding integrals. The above algorithm also improves the search time com- pared to a direct binary search approach. In the following, we present several explicit examples to show the effectiveness of Ellipse-type priority functions. We will first show the examples with single target inte- ...

  6. [6]

    K. G. Chetyrkin and F. V. Tkachov, Nucl. Phys. B 192, 159 (1981)

  7. [7]

    F. V. Tkachov, Phys. Lett. B 100, 65 (1981). 11

  8. [8]

    A. V. Kotikov, Phys. Lett. B 254, 158 (1991)

Show all 95 references
  1. [9]

    Gehrmann and E

    T. Gehrmann and E. Remiddi, Nucl. Phys. B 580, 485 (2000), arXiv:hep-ph/9912329

  2. [10]

    J. M. Henn, Phys. Rev. Lett. 110, 251601 (2013), arXiv:1304.1806 [hep-th]

  3. [11]

    Laporta, Int

    S. Laporta, Int. J. Mod. Phys. A 15, 5087 (2000), arXiv:hep-ph/0102033

  4. [12]

    von Manteuffel and R

    A. von Manteuffel and R. M. Schabinger, Phys. Lett. B 744, 101 (2015), arXiv:1406.4513 [hep-ph]

  5. [13]

    Peraro, JHEP 12, 030 (2016), arXiv:1608.01902 [hep- ph]

    T. Peraro, JHEP 12, 030 (2016), arXiv:1608.01902 [hep- ph]

  6. [14]

    Gluza, K

    J. Gluza, K. Kajda, and D. A. Kosower, Phys. Rev. D 83, 045012 (2011), arXiv:1009.0472 [hep-th]

  7. [15]

    K. J. Larsen and Y. Zhang, Phys. Rev. D 93, 041701 (2016), arXiv:1511.01071 [hep-th]

  8. [16]

    B¨ ohm, A

    J. B¨ ohm, A. Georgoudis, K. J. Larsen, M. Schulze, and Y. Zhang, Phys. Rev. D 98, 025023 (2018), arXiv:1712.09737 [hep-th]

  9. [17]

    R. N. Lee, in 49th Rencontres de Moriond on QCD and High Energy Interactions (2014) pp. 297–300, arXiv:1405.5616 [hep-ph]

  10. [18]

    Bitoun, C

    T. Bitoun, C. Bogner, R. P. Klausen, and E. Panzer, Lett. Math. Phys. 109, 497 (2019), arXiv:1712.09215 [hep-th]

  11. [19]

    Agarwal, S

    B. Agarwal, S. P. Jones, and A. von Manteuffel, JHEP 05, 256 (2021), arXiv:2011.15113 [hep-ph]

  12. [20]

    Mastrolia and S

    P. Mastrolia and S. Mizera, JHEP 02, 139 (2019), arXiv:1810.03818 [hep-th]

  13. [21]

    Frellesvig, F

    H. Frellesvig, F. Gasparotto, M. K. Mandal, P. Mastro- lia, L. Mattiazzi, and S. Mizera, Phys. Rev. Lett. 123, 201602 (2019), arXiv:1907.02000 [hep-th]

  14. [22]

    Liu and Y.-Q

    X. Liu and Y.-Q. Ma, Phys. Rev. D 99, 071501 (2019), arXiv:1801.10523 [hep-ph]

  15. [23]

    X. Guan, X. Liu, and Y.-Q. Ma, Chin. Phys. C 44, 093106 (2020), arXiv:1912.09294 [hep-ph]

  16. [24]

    X. Guan, X. Liu, Y.-Q. Ma, and W.-H. Wu, (2024), arXiv:2405.14621 [hep-ph]

  17. [25]

    Anastasiou and A

    C. Anastasiou and A. Lazopoulos, JHEP 07, 046 (2004), arXiv:hep-ph/0404258

  18. [26]

    R. N. Lee, (2012), arXiv:1212.2685 [hep-ph]

  19. [27]

    R. N. Lee, J. Phys. Conf. Ser. 523, 012059 (2014), arXiv:1310.1145 [hep-ph]

  20. [28]

    A. V. Smirnov and F. S. Chukharev, Comput. Phys. Commun. 247, 106877 (2020), arXiv:1901.07808 [hep- ph]

  21. [29]

    A. V. Smirnov and M. Zeng, Comput. Phys. Commun. 302, 109261 (2024), arXiv:2311.02370 [hep-ph]

  22. [30]

    von Manteuffel and C

    A. von Manteuffel and C. Studerus, (2012), arXiv:1201.4330 [hep-ph]

  23. [31]

    Studerus, Comput

    C. Studerus, Comput. Phys. Commun. 181, 1293 (2010), arXiv:0912.2546 [physics.comp-ph]

  24. [32]

    Maierh¨ ofer, J

    P. Maierh¨ ofer, J. Usovitsch, and P. Uwer, Comput. Phys. Commun. 230, 99 (2018), arXiv:1705.05610 [hep-ph]

  25. [33]

    Klappert and F

    J. Klappert and F. Lange, Comput. Phys. Commun. 247, 106951 (2020), arXiv:1904.00009 [cs.SC]

  26. [34]

    Klappert, F

    J. Klappert, F. Lange, P. Maierh¨ ofer, and J. Uso- vitsch, Comput. Phys. Commun. 266, 108024 (2021), arXiv:2008.06494 [hep-ph]

  27. [35]

    Ruijl, T

    B. Ruijl, T. Ueda, and J. A. M. Vermaseren, Comput. Phys. Commun. 253, 107198 (2020), arXiv:1704.06650 [hep-ph]

  28. [36]

    Peraro, JHEP 07, 031 (2019), arXiv:1905.08019 [hep- ph]

    T. Peraro, JHEP 07, 031 (2019), arXiv:1905.08019 [hep- ph]

  29. [37]

    Z. Wu, J. Boehm, R. Ma, H. Xu, and Y. Zhang, Comput. Phys. Commun. 295, 108999 (2024), arXiv:2305.08783 [hep-ph]

  30. [38]

    Chen, (2024), arXiv:2408.06426 [hep-ph]

    W. Chen, (2024), arXiv:2408.06426 [hep-ph]

  31. [39]

    Romera-Paredes, M

    B. Romera-Paredes, M. Barekatain, A. Novikov, M. Ba- log, M. P. Kumar, E. Dupont, F. J. Ruiz, J. S. Ellenberg, P. Wang, O. Fawzi, et al., Nature 625, 468 (2024)

  32. [40]

    He, Nature Rev

    Y.-H. He, Nature Rev. Phys. 6, 546 (2024), arXiv:2405.19973 [math.HO]

  33. [41]

    He, ed., Machine Learning in Pure Mathematics and Theoretical Physics(World Scientific, 2023)

    Y.-H. He, ed., Machine Learning in Pure Mathematics and Theoretical Physics(World Scientific, 2023)

  34. [42]

    He and S.-J

    Y.-H. He and S.-J. Lee, Phys. Lett. B798, 134889 (2019), arXiv:1904.08530 [hep-th]

  35. [43]

    Y.-H. He, Int. J. Mod. Phys. A 36, 2130017 (2021), arXiv:2011.14442 [hep-th]

  36. [44]

    T. Cai, G. W. Merz, F. Charton, N. Nolte, M. Wilhelm, K. Cranmer, and L. J. Dixon, Mach. Learn. Sci. Tech. 5, 035073 (2024), arXiv:2405.06107 [cs.LG]

  37. [45]

    L. J. Dixon, O. Gurdogan, A. J. McLeod, and M. Wil- helm, JHEP 07, 153 (2022), arXiv:2204.11901 [hep-th]

  38. [46]

    M. D. Schwartz, (2021), 10.1162/99608f92.beeb1183, arXiv:2103.12226 [hep-ph]

  39. [47]

    Dersy, M

    A. Dersy, M. D. Schwartz, and X. Zhang, Int. J. Data Sci. Math. Sci. 1, 135 (2024), arXiv:2206.04115 [cs.LG]

  40. [48]

    Dersy, M

    A. Dersy, M. D. Schwartz, and A. Zhiboedov, JHEP 05, 200 (2024), arXiv:2308.09451 [hep-th]

  41. [49]

    Cheung, A

    C. Cheung, A. Dersy, and M. D. Schwartz, SciPost Phys. 18, 040 (2025), arXiv:2408.04720 [hep-th]

  42. [50]

    Demirtas, J

    M. Demirtas, J. Halverson, A. Maiti, M. D. Schwartz, and K. Stoner, Mach. Learn. Sci. Tech. 5, 015002 (2024), arXiv:2307.03223 [hep-th]

  43. [51]

    Bhattacharya, J

    A. Bhattacharya, J. Cotler, A. Dersy, and M. D. Schwartz, Phys. Rev. D 110, 116023 (2024), arXiv:2402.18633 [hep-th]

  44. [52]

    P. T. Komiske, E. M. Metodiev, and M. D. Schwartz, JHEP 01, 110 (2017), arXiv:1612.01551 [hep-ph]

  45. [53]

    P. T. Komiske, E. M. Metodiev, B. Nachman, and M. D. Schwartz, JHEP 12, 051 (2017), arXiv:1707.08600 [hep- ph]

  46. [54]

    Heimel, G

    T. Heimel, G. Kasieczka, T. Plehn, and J. M. Thompson, SciPost Phys. 6, 030 (2019), arXiv:1808.08979 [hep-ph]

  47. [55]

    Qu and L

    H. Qu and L. Gouskos, Phys. Rev. D 101, 056019 (2020), arXiv:1902.08570 [hep-ph]

  48. [56]

    S. Gong, Q. Meng, J. Zhang, H. Qu, C. Li, S. Qian, W. Du, Z.-M. Ma, and T.-Y. Liu, JHEP 07, 030 (2022), arXiv:2201.08187 [hep-ph]

  49. [57]

    Bright-Thonney, B

    S. Bright-Thonney, B. Nachman, and J. Thaler, Phys. Rev. D 110, 014029 (2024), arXiv:2311.07652 [hep-ph]

  50. [58]

    E. M. Metodiev, J. Thaler, and R. Wynne, Phys. Rev. D 110, 055012 (2024), arXiv:2312.00119 [hep-ph]

  51. [59]

    Desai, B

    K. Desai, B. Nachman, and J. Thaler, Phys. Rev. D 110, 116013 (2024), arXiv:2407.11284 [hep-ph]

  52. [60]

    Gambhir, A

    R. Gambhir, A. Osathapan, and J. Thaler, Phys. Rev. D 110, 074020 (2024), arXiv:2403.08854 [hep-ph]

  53. [61]

    Heimel, N

    T. Heimel, N. Huetsch, R. Winterhalder, T. Plehn, and A. Butter, SciPost Phys. 17, 129 (2024), arXiv:2310.07752 [hep-ph]

  54. [62]

    Badger et al

    S. Badger et al. , SciPost Phys. 14, 079 (2023), arXiv:2203.07460 [hep-ph]

  55. [63]

    Forte, L

    S. Forte, L. Garrido, J. I. Latorre, and A. Piccione, JHEP 05, 062 (2002), arXiv:hep-ph/0204232

  56. [64]

    R. D. Ball et al. (NNPDF), JHEP 04, 040 (2015), arXiv:1410.8849 [hep-ph]

  57. [65]

    D. Liu, C. Sun, and J. Gao, JHEP 08, 088 (2022), arXiv:2201.06586 [hep-ph]. 12

  58. [66]

    Badger and J

    S. Badger and J. Bullock, JHEP 06, 114 (2020), arXiv:2002.07516 [hep-ph]

  59. [67]

    Aylett-Bullock, S

    J. Aylett-Bullock, S. Badger, and R. Moodie, JHEP 08, 066 (2021), arXiv:2106.09474 [hep-ph]

  60. [68]

    Fedkevych, C

    O. Fedkevych, C. K. Khosa, S. Marzani, and F. Sforza, Phys. Rev. D 107, 034032 (2023), arXiv:2202.05082 [hep- ph]

  61. [69]

    Calisto, R

    F. Calisto, R. Moodie, and S. Zoia, JHEP 07, 124 (2024), arXiv:2312.02067 [hep-ph]

  62. [70]

    Halverson and F

    J. Halverson and F. Ruehle, Physical Review D 99, 046015 (2019)

  63. [71]

    Gukov, J

    S. Gukov, J. Halverson, F. Ruehle, and P. Su lkowski, Machine Learning: Science and Technology 2, 025035 (2021)

  64. [72]

    Halverson, A

    J. Halverson, A. Maiti, and K. Stoner, Machine Learn- ing: Science and Technology 2, 035002 (2021)

  65. [73]

    Halverson, B

    J. Halverson, B. Nelson, and F. Ruehle, Journal of High Energy Physics 2019, 1 (2019)

  66. [74]

    Carifio, J

    J. Carifio, J. Halverson, D. Krioukov, and B. D. Nelson, Journal of High Energy Physics 2017, 1 (2017)

  67. [75]

    V. A. Smirnov, Analytic Tools for Feynman Integrals, Springer Tracts in Modern Physics, Vol. 250 (Springer, 2012)

  68. [76]

    Anastasiou and K

    C. Anastasiou and K. Melnikov, Nucl. Phys. B 646, 220 (2002), arXiv:hep-ph/0207004

  69. [77]

    Driesse, G

    M. Driesse, G. U. Jakobsen, G. Mogull, J. Plefka, B. Sauer, and J. Usovitsch, Phys. Rev. Lett. 132, 241402 (2024), arXiv:2403.07781 [hep-th]

  70. [78]

    Z. Bern, E. Herrmann, R. Roiban, M. S. Ruf, A. V. Smirnov, V. A. Smirnov, and M. Zeng, JHEP 10, 023 (2024), arXiv:2406.01554 [hep-th]

  71. [79]

    Hsevo: Ele- vating automatic heuristic design with diversity-driven harmony search and genetic algorithm using llms,

    P. V. T. Dat, L. Doan, and H. T. T. Binh, “Hsevo: Ele- vating automatic heuristic design with diversity-driven harmony search and genetic algorithm using llms,” (2024), arXiv:2412.14995 [cs.NE]

  72. [80]

    Evolution of heuristics: Towards efficient automatic algorithm design using large language model,

    F. Liu, X. Tong, M. Yuan, X. Lin, F. Luo, Z. Wang, Z. Lu, and Q. Zhang, “Evolution of heuristics: Towards efficient automatic algorithm design using large language model,” (2024), arXiv:2401.02051 [cs.NE]

  73. [81]

    Reevo: Large language mod- els as hyper-heuristics with reflective evolution,

    H. Ye, J. Wang, Z. Cao, F. Berto, C. Hua, H. Kim, J. Park, and G. Song, “Reevo: Large language mod- els as hyper-heuristics with reflective evolution,” (2024), arXiv:2402.01145 [cs.NE]

  74. [82]

    Uber: Uncertainty-based evolution with large lan- guage models for automatic heuristic design,

    Z. Chen, Z. Zhou, Y. Lu, R. Xu, L. Pan, and Z. Lan, “Uber: Uncertainty-based evolution with large lan- guage models for automatic heuristic design,” (2024), arXiv:2412.20694 [cs.NE]

  75. [83]

    Monte carlo tree search for comprehensive exploration in llm-based automatic heuristic design,

    Z. Zheng, Z. Xie, Z. Wang, and B. Hooi, “Monte carlo tree search for comprehensive exploration in llm-based automatic heuristic design,” (2025), arXiv:2501.08603 [cs.AI]

  76. [84]

    Funbo: Dis- covering acquisition functions for bayesian optimization with funsearch,

    V. Aglietti, I. Ktena, J. Schrouff, E. Sgouritsa, F. J. R. Ruiz, A. Malek, A. Bellot, and S. Chiappa, “Funbo: Dis- covering acquisition functions for bayesian optimization with funsearch,” (2024), arXiv:2406.04824 [cs.LG]

  77. [85]

    Understanding the importance of evolutionary search in automated heuristic design with large language models,

    R. Zhang, F. Liu, X. Lin, Z. Wang, Z. Lu, and Q. Zhang, “Understanding the importance of evolutionary search in automated heuristic design with large language models,” (2024), arXiv:2407.10873 [cs.NE]

  78. [86]

    Gituliar, V

    O. Gituliar, V. Magerya, and A. Pikelner, JHEP 06, 099 (2018), arXiv:1803.09084 [hep-ph]

  79. [87]

    Magerya and A

    V. Magerya and A. Pikelner, JHEP 12, 026 (2019), arXiv:1910.07522 [hep-ph]

  80. [88]

    Maheria, Semi- and Fully-Inclusive Phase-Space Inte- grals at Four Loops, Ph.D

    V. Maheria, Semi- and Fully-Inclusive Phase-Space Inte- grals at Four Loops, Ph.D. thesis, Hamburg U. (2022)

  81. [89]

    O. V. Tarasov, Phys. Rev. D 54, 6479 (1996), arXiv:hep- th/9606018

  82. [90]

    Refining integration-by- parts reduction of feynman integrals with machine learn- ing,

    M. von Hippel and M. Wilhelm, “Refining integration-by- parts reduction of feynman integrals with machine learn- ing,” (2025), arXiv:2502.05121 [hep-th]

  83. [91]

    Minicpm: Unveiling the potential of small lan- guage models with scalable training strategies,

    S. Hu, Y. Tu, X. Han, C. He, G. Cui, X. Long, Z. Zheng, Y. Fang, Y. Huang, W. Zhao, X. Zhang, Z. L. Thai, K. Zhang, C. Wang, Y. Yao, C. Zhao, J. Zhou, J. Cai, Z. Zhai, N. Ding, C. Jia, G. Zeng, D. Li, Z. Liu, and M. Sun, “Minicpm: Unveiling the potential of small lan- guage mo...

  84. [92]

    Qwen technical report,

    J. Bai, S. Bai, Y. Chu, Z. Cui, K. Dang, X. Deng, Y. Fan, W. Ge, Y. Han, F. Huang, B. Hui, L. Ji, M. Li, J. Lin, R. Lin, D. Liu, G. Liu, C. Lu, K. Lu, J. Ma, R. Men, X. Ren, X. Ren, C. Tan, S. Tan, J. Tu, P. Wang, S. Wang, W. Wang, S. Wu, B. Xu, J. Xu, A. Yang, H. Yang, J. Yan...

  85. [93]

    Below lists some key hyperparameters and their selection criteria: Model: The CPM-2B model [86] was selected due to its superior performance in code generation tasks

    Hyperparameter Selection The selection of hyperparameters significantly impacts the performance and outcomes of FunSearch. Below lists some key hyperparameters and their selection criteria: Model: The CPM-2B model [86] was selected due to its superior performance in code gener...

  86. [94]

    The initial seeding employed was the Laporta priority 2

    Brief Analysis of the Evolution Process In the experiments, we executed FunSearch for one- loop IBP reductions a total of 10 times, with each run comprising 5000 epochs. The initial seeding employed was the Laporta priority 2. During each epoch, the pri- ority function was eva...

  87. [95]

    , y - node [1]]) ** 2 + node [0] ** 2 + node [1] ** 2 for x , y in n o d e _ t a r g e t s ) ) Its expanded form is given by: F0(I(ni);Itargetj(tji)) = − "X n2 i + max j X i (ni − tji)2 !# . (B1) This result indicates that even with multiple target points, the algorithm was ab...

Pith tools

Reviewed August 7, 2026 · model on record in the stance chip above.