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arxiv: 2604.25270 · v1 · submitted 2026-04-28 · ✦ hep-th · hep-ph

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Integrand Analysis, Leading Singularities and Canonical Bases beyond Polylogarithms

Authors on Pith no claims yet

Pith reviewed 2026-05-07 16:01 UTC · model grok-4.3

classification ✦ hep-th hep-ph
keywords leading singularitiesFeynman integralscanonical basesepsilon-factorized differential equationsGauss-Manin connectiontranscendental functionsperiodspolylogarithms
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0 comments X

The pith

Selecting Feynman integrals with unit leading singularities in generalized geometries produces ε-factorized differential equations and new transcendental functions tied to periods.

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

The paper develops a way to extend leading singularities and canonical bases for Feynman integrals past the polylogarithmic regime. It generalizes the notion of leading singularities from the Riemann sphere to more involved geometries inside dimensional regularization. Choosing integrals that carry unit leading singularities in this broader setting forces the appearance of new transcendental functions built from the periods of those geometries. The resulting integrals obey ε-factorized differential equations whose new forms match the extra differential forms in the associated Gauss-Manin connection. The construction is presented as equivalent to decomposing the period matrix into semi-simple and unipotent pieces plus a clean-up step, with concrete examples that mix several geometries.

Core claim

We elaborate on the connection between leading singularities and canonical bases of Feynman integrals beyond polylogarithms. We start by discussing a notion of leading singularities in dimensional regularization, which can be generalized from the Riemann sphere to more complex geometries, and use it to demonstrate how selecting Feynman integrals with unit leading singularities necessitates introducing new transcendental functions related to the periods of the underlying geometries. Integrals with unit leading singularities in this generalized sense satisfy ε-factorized differential equations, and the new transcendental functions are in direct correspondence to the new differential forms in a

What carries the argument

The generalized leading singularity defined on complex geometries in dimensional regularization, which selects integrals whose differential equations factorize in ε and whose new transcendental parts match the additional differential forms of the Gauss-Manin connection.

If this is right

  • Feynman integrals beyond polylogarithms admit canonical bases built by the unit-leading-singularity criterion.
  • New transcendental functions appear that are directly linked to the periods of the underlying geometries.
  • The differential equations satisfied by these integrals become ε-factorized, reducing the complexity of their integration.
  • The method works for examples that involve the interplay of several distinct geometries.
  • The procedure is mathematically equivalent to splitting the period matrix into semi-simple and unipotent parts followed by a clean-up.

Where Pith is reading between the lines

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

  • The same selection rule may supply a practical route to canonical bases for multi-loop amplitudes whose kinematics involve higher-genus surfaces or other non-rational geometries.
  • It could tighten the link between Feynman-integral techniques and the algebraic-geometry study of periods and Gauss-Manin connections.
  • Testing the construction on concrete higher-order processes in QCD or gravity would reveal whether the new functions can be evaluated numerically or reduced to known constants.
  • Further work might explore whether the same geometric splitting applies to integrals whose leading singularities live on even more intricate varieties.

Load-bearing premise

A notion of leading singularities can be extended from the Riemann sphere to more complex geometries while keeping the property that unit leading singularities still produce ε-factorized differential equations.

What would settle it

An explicit Feynman integral that possesses a unit leading singularity under the generalized definition yet fails to obey an ε-factorized differential equation, or whose solution requires transcendental functions that do not correspond to the periods of the geometry.

read the original abstract

In this paper, we elaborate on the connection between leading singularities and canonical bases of Feynman integrals beyond polylogarithms. We start by discussing a notion of leading singularities in dimensional regularization, which can be generalized from the Riemann sphere to more complex geometries, and use it to demonstrate how selecting Feynman integrals with unit leading singularities necessitates introducing new transcendental functions related to the periods of the underlying geometries. Integrals with unit leading singularities in this generalized sense, satisfy $\epsilon$-factorized differential equations, and the new transcendental functions are in direct correspondence to the new differential forms appearing in their Gauss-Manin connection. We argue that this construction is mathematically equivalent to the splitting of the period matrix into semi-simple and unipotent parts plus a clean-up step, and demonstrate its use with examples of increasing complexity that require the interplay of multiple geometries.

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

1 major / 1 minor

Summary. The paper elaborates on the connection between leading singularities and canonical bases of Feynman integrals beyond polylogarithms. It generalizes the notion of leading singularities in dimensional regularization from the Riemann sphere to more complex geometries. Selecting integrals with unit leading singularities requires introducing new transcendental functions related to the periods of the underlying geometries. Such integrals satisfy ε-factorized differential equations, with the new functions in direct correspondence to new differential forms in the Gauss-Manin connection. The construction is argued to be mathematically equivalent to splitting the period matrix into semi-simple and unipotent parts plus a clean-up step, and is demonstrated with examples of increasing complexity involving multiple geometries.

Significance. If the generalization holds rigorously, the work would offer a systematic approach to canonical bases for Feynman integrals involving higher transcendental functions, with potential impact on multi-loop amplitude computations in QFT. The claimed mathematical equivalence to period-matrix splitting provides a possible bridge to algebraic geometry methods, and the use of examples with multiple geometries is a constructive step. However, the absence of a general theorem (as opposed to example-based demonstration) limits the assessed significance at present.

major comments (1)
  1. [Abstract] Abstract: The assertion that the construction is mathematically equivalent to the splitting of the period matrix into semi-simple and unipotent parts plus a clean-up step is load-bearing for the central claim of a reliable generalization. The abstract states the equivalence but provides no indication of the section, derivation, or proof strategy establishing it in general (rather than for the specific examples of increasing complexity). This leaves open whether ε-factorization and the 1-1 correspondence to Gauss-Manin forms are preserved when multiple geometries interplay without additional assumptions.
minor comments (1)
  1. The abstract would benefit from a short statement of the specific examples used and the geometries involved, to better orient the reader before the full text.

Simulated Author's Rebuttal

1 responses · 1 unresolved

We thank the referee for their careful reading of the manuscript and for the constructive feedback on the abstract's presentation of the central claim. We address the major comment point by point below.

read point-by-point responses
  1. Referee: [Abstract] Abstract: The assertion that the construction is mathematically equivalent to the splitting of the period matrix into semi-simple and unipotent parts plus a clean-up step is load-bearing for the central claim of a reliable generalization. The abstract states the equivalence but provides no indication of the section, derivation, or proof strategy establishing it in general (rather than for the specific examples of increasing complexity). This leaves open whether ε-factorization and the 1-1 correspondence to Gauss-Manin forms are preserved when multiple geometries interplay without additional assumptions.

    Authors: We agree that the abstract would benefit from explicitly indicating the location and nature of the argument for the claimed equivalence. In the manuscript, the mathematical equivalence to the semi-simple/unipotent splitting of the period matrix (plus clean-up) is derived and argued in Section 3, where we show how the generalized leading-singularity condition selects the semi-simple part while the unipotent contributions are isolated and removed. This derivation directly implies the preservation of ε-factorization and the one-to-one correspondence with the new differential forms in the Gauss-Manin connection. Sections 4 and 5 then apply the procedure to cases with multiple interacting geometries, explicitly verifying that the ε-factorized form and the correspondence are maintained. We will revise the abstract to reference Section 3 for the derivation and to clarify that the equivalence is established as a general construction, demonstrated through examples of increasing complexity. We note that the paper presents this as an argued procedure supported by explicit verification rather than a standalone general theorem; a fully rigorous proof for arbitrary geometries would constitute additional mathematical work beyond the scope of the current manuscript. revision: partial

standing simulated objections not resolved
  • Providing a rigorous general theorem (as opposed to an argued construction verified by explicit examples) establishing the equivalence and preservation of ε-factorization for arbitrary multiple geometries without further assumptions.

Circularity Check

0 steps flagged

No circularity: generalization and equivalence presented as independent mathematical argument supported by examples

full rationale

The paper defines a generalized notion of leading singularities in dimensional regularization, shows that unit leading singularities imply ε-factorized differential equations with new transcendentals corresponding to Gauss-Manin forms, and separately argues that this construction is mathematically equivalent to splitting the period matrix into semi-simple and unipotent parts plus a clean-up step. This equivalence is stated as an argument and demonstrated via examples of increasing complexity, without any quoted reduction of the central claim to a fitted parameter, self-definition, or load-bearing self-citation that collapses the result to its inputs by construction. The derivation chain remains self-contained against external benchmarks such as the stated mathematical equivalence and explicit examples.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Based on the abstract, no explicit free parameters, axioms, or invented entities are detailed; the work relies on generalizations of existing concepts in Feynman integral calculus and algebraic geometry.

pith-pipeline@v0.9.0 · 5451 in / 1103 out tokens · 55392 ms · 2026-05-07T16:01:51.786779+00:00 · methodology

discussion (0)

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Reference graph

Works this paper leans on

72 extracted references · 65 canonical work pages · 2 internal anchors

  1. [1]

    Arkani-Hamed, J.L

    N. Arkani-Hamed, J.L. Bourjaily, F. Cachazo and J. Trnka,Local Integrals for Planar Scattering Amplitudes,JHEP06(2012) 125 [1012.6032]

  2. [2]

    Henn,Multiloop integrals in dimensional regularization made simple,Phys

    J.M. Henn,Multiloop integrals in dimensional regularization made simple,Phys. Rev. Lett. 110(2013) 251601 [1304.1806]

  3. [3]

    Kummer,Über die Transcendenten, welche aus wiederholten Integrationen rationaler Formeln entstehen,J

    E.E. Kummer,Über die Transcendenten, welche aus wiederholten Integrationen rationaler Formeln entstehen,J. reine ang. Mathematik21(1840) 74

  4. [4]

    Goncharov,Geometry of configurations, polylogarithms, and motivic cohomology, Adv

    A.B. Goncharov,Geometry of configurations, polylogarithms, and motivic cohomology, Adv. Math.114(1995) 197

  5. [5]

    Harmonic Polylogarithms

    E. Remiddi and J.A.M. Vermaseren,Harmonic polylogarithms,Int. J. Mod. Phys.A15 (2000) 725 [hep-ph/9905237]

  6. [6]

    Gehrmann and E

    T. Gehrmann and E. Remiddi,Differential equations for two-loop four-point functions,Nucl. Phys. B580(2000) 485 [hep-ph/9912329]

  7. [7]

    Goncharov, M

    A.B. Goncharov, M. Spradlin, C. Vergu and A. Volovich,Classical Polylogarithms for Amplitudes and Wilson Loops,Phys. Rev. Lett.105(2010) 151605 [1006.5703]

  8. [8]

    C. Duhr, H. Gangl and J.R. Rhodes,From polygons and symbols to polylogarithmic functions,JHEP1210(2012) 075 [1110.0458]

  9. [9]

    Duhr,Hopf algebras, coproducts and symbols: an application to Higgs boson amplitudes, JHEP08(2012) 043 [1203.0454]

    C. Duhr,Hopf algebras, coproducts and symbols: an application to Higgs boson amplitudes, JHEP08(2012) 043 [1203.0454]

  10. [10]

    ’t Hooft and M.J.G

    G. ’t Hooft and M.J.G. Veltman,Regularization and Renormalization of Gauge Fields,Nucl. Phys. B44(1972) 189

  11. [11]

    Bollini and J.J

    C.G. Bollini and J.J. Giambiagi,Dimensional Renormalization: The Number of Dimensions as a Regularizing Parameter,Nuovo Cim. B12(1972) 20. – 44 –

  12. [12]

    Kotikov,Differential equations method: New technique for massive Feynman diagrams calculation,Phys

    A.V. Kotikov,Differential equations method: New technique for massive Feynman diagrams calculation,Phys. Lett. B254(1991) 158

  13. [13]

    Remiddi,Differential equations for Feynman graph amplitudes,Nuovo Cim

    E. Remiddi,Differential equations for Feynman graph amplitudes,Nuovo Cim. A110(1997) 1435 [hep-th/9711188]

  14. [14]

    Cachazo,Sharpening The Leading Singularity,0803.1988

    F. Cachazo,Sharpening The Leading Singularity,0803.1988

  15. [15]

    J. Henn, B. Mistlberger, V.A. Smirnov and P. Wasser,Constructing d-log integrands and computing master integrals for three-loop four-particle scattering,JHEP04(2020) 167 [2002.09492]

  16. [16]

    Adams, C

    L. Adams, C. Bogner, A. Schweitzer and S. Weinzierl,The kite integral to all orders in terms of elliptic polylogarithms,J. Math. Phys.57(2016) 122302 [1607.01571]

  17. [17]

    Adams and S

    L. Adams and S. Weinzierl,Theε-form of the differential equations for Feynman integrals in the elliptic case,Phys. Lett. B781(2018) 270 [1802.05020]

  18. [18]

    Dlapa, J.M

    C. Dlapa, J.M. Henn and F.J. Wagner,An algorithmic approach to finding canonical differential equations for elliptic Feynman integrals,JHEP08(2023) 120 [2211.16357]

  19. [19]

    Yang and Y

    L.L. Yang and Y. Zhang,FromdlogtodE: Canonical Elliptic Integrands and Modular Symbol Letters with Pure eMPLs,2512.19370

  20. [20]

    Chaubey and V

    E. Chaubey and V. Sotnikov,Elliptic Leading Singularities and Canonical Integrands,Phys. Rev. Lett.135(2025) 101903 [2504.20897]

  21. [21]

    Chen, L.L

    J. Chen, L.L. Yang and Y. Zhang,On an approach to canonicalizing elliptic Feynman integrals,2503.23720

  22. [22]

    Adams, E

    L. Adams, E. Chaubey and S. Weinzierl,Planar Double Box Integral for Top Pair Production with a Closed Top Loop to all orders in the Dimensional Regularization Parameter,Phys. Rev. Lett.121(2018) 142001 [1804.11144]

  23. [23]

    Pögel, X

    S. Pögel, X. Wang and S. Weinzierl,Taming Calabi-Yau Feynman Integrals: The Four-Loop Equal-Mass Banana Integral,Phys. Rev. Lett.130(2023) 101601 [2211.04292]

  24. [24]

    Pögel, X

    S. Pögel, X. Wang and S. Weinzierl,Bananas of equal mass: any loop, any order in the dimensional regularisation parameter,JHEP04(2023) 117 [2212.08908]

  25. [25]

    Pögel, X

    S. Pögel, X. Wang and S. Weinzierl,The three-loop equal-mass banana integral inε-factorised form with meromorphic modular forms,JHEP09(2022) 062 [2207.12893]

  26. [26]

    Görges, C

    L. Görges, C. Nega, L. Tancredi and F.J. Wagner,On a procedure to deriveϵ-factorised differential equations beyond polylogarithms,JHEP07(2023) 206 [2305.14090]

  27. [27]

    C. Duhr, F. Porkert and S.F. Stawinski,Canonical differential equations beyond genus one, JHEP02(2025) 014 [2412.02300]

  28. [28]

    C. Duhr, S. Maggio, C. Nega, B. Sauer, L. Tancredi and F.J. Wagner,Aspects of canonical differential equations for Calabi-Yau geometries and beyond,JHEP06(2025) 128 [2503.20655]

  29. [29]

    Maggio and Y

    S. Maggio and Y. Sohnle,On canonical differential equations for Calabi-Yau multi-scale Feynman integrals,JHEP10(2025) 202 [2504.17757]. [30]ε-collaborationcollaboration,The geometric bookkeeping guide to Feynman integral reduction andε-factorised differential equations,2506.09124. – 45 –

  30. [30]

    New algorithms for Feynman integral reduction and $\varepsilon$-factorised differential equations

    I. Bree et al.,New algorithms for Feynman integral reduction andε-factorised differential equations,2511.15381

  31. [31]

    Frellesvig,On epsilon factorized differential equations for elliptic Feynman integrals, JHEP03(2022) 079 [2110.07968]

    H. Frellesvig,On epsilon factorized differential equations for elliptic Feynman integrals, JHEP03(2022) 079 [2110.07968]

  32. [32]

    Frellesvig and S

    H. Frellesvig and S. Weinzierl,Onε-factorised bases and pure Feynman integrals,SciPost Phys.16(2024) 150 [2301.02264]

  33. [33]

    Jiang, X

    X. Jiang, X. Wang, L.L. Yang and J. Zhao,ε-factorized differential equations for two-loop non-planar triangle Feynman integrals with elliptic curves,JHEP09(2023) 187 [2305.13951]

  34. [34]

    Giroux, A

    M. Giroux, A. Pokraka, F. Porkert and Y. Sohnle,The soaring kite: a tale of two punctured tori,JHEP05(2024) 239 [2401.14307]

  35. [35]

    Marzucca, A.J

    R. Marzucca, A.J. McLeod and C. Nega,Two-Loop Master Integrals for Mixed QCD-EW Corrections togg→HThroughO(ϵ 2),2501.14435

  36. [36]

    Becchetti, F

    M. Becchetti, F. Coro, C. Nega, L. Tancredi and F.J. Wagner,Analytic two-loop amplitudes forq q→γγand gg→γγmediated by a heavy-quark loop,JHEP06(2025) 033 [2502.00118]

  37. [37]

    Becchetti, C

    M. Becchetti, C. Dlapa and S. Zoia,Canonical differential equations for the elliptic two-loop five-point integral family relevant tot¯t+jet production at leading colour,2503.03603

  38. [38]

    F. Coro, C. Nega, L. Tancredi and F.J. Wagner,Analytic two-loop amplitudes for di-jet and γ+jet production mediated by a heavy-quark loop,JHEP01(2026) 090 [2509.15315]

  39. [39]

    C. Duhr, A. Klemm, F. Loebbert, C. Nega and F. Porkert,Yangian-Invariant Fishnet Integrals in Two Dimensions as Volumes of Calabi-Yau Varieties,Phys. Rev. Lett.130 (2023) 041602 [2209.05291]

  40. [40]

    C. Duhr, A. Klemm, F. Loebbert, C. Nega and F. Porkert,The Basso-Dixon formula and Calabi-Yau geometry,JHEP03(2024) 177 [2310.08625]

  41. [41]

    C. Duhr, A. Klemm, F. Loebbert, C. Nega and F. Porkert,Geometry from integrability: multi-leg fishnet integrals in two dimensions,JHEP07(2024) 008 [2402.19034]

  42. [42]

    C. Duhr, F. Gasparotto, C. Nega, L. Tancredi and S. Weinzierl,On the electron self-energy to three loops in QED,JHEP11(2024) 020 [2408.05154]

  43. [43]

    Forner, C

    F. Forner, C. Nega and L. Tancredi,On the photon self-energy to three loops in QED, 2411.19042

  44. [44]

    C. Duhr, S. Maggio, F. Porkert, C. Semper and S.F. Stawinski,Three-loop banana integrals with four unequal masses,JHEP12(2025) 034 [2507.23061]

  45. [45]

    Duhr and S

    C. Duhr and S. Maggio,Three-loop banana integrals with three equal masses,2511.19245

  46. [46]

    Pögel, T

    S. Pögel, T. Teschke, X. Wang and S. Weinzierl,The unequal-mass three-loop banana integral,JHEP01(2026) 021 [2507.23594]

  47. [47]

    Z. Bern, E. Herrmann, R. Roiban, M.S. Ruf, A.V. Smirnov, S. Smith et al.,Scattering Amplitudes and Conservative Binary Dynamics atO(G5)without Self-Force Truncation, 2512.23654

  48. [48]

    Klemm, C

    A. Klemm, C. Nega, B. Sauer and J. Plefka,Calabi-Yau periods for black hole scattering in classical general relativity,Phys. Rev. D109(2024) 124046 [2401.07899]. – 46 –

  49. [49]

    Driesse, G

    M. Driesse, G.U. Jakobsen, A. Klemm, G. Mogull, C. Nega, J. Plefka et al.,High-precision black hole scattering with Calabi-Yau manifolds,2411.11846

  50. [50]

    Driesse, G

    M. Driesse, G.U. Jakobsen, G. Mogull, C. Nega, J. Plefka, B. Sauer et al.,Conservative Black Hole Scattering at Fifth Post-Minkowskian and Second Self-Force Order,2601.16256

  51. [51]

    Z. Bern, A. Jackman, G. Mansfield and M.S. Ruf,Classical Gravitational Scattering from the Ultraviolet and the Absence of Calabi-Yau Integrals in the Conservative Sector atO(G5), 2603.15383

  52. [52]

    Leading Singularity

    J.L. Bourjaily, N. Kalyanapuram, C. Langer, K. Patatoukos and M. Spradlin,Elliptic, Yangian-Invariant “Leading Singularity”,Phys. Rev. Lett.126(2021) 201601 [2012.14438]

  53. [53]

    Bourjaily, N

    J.L. Bourjaily, N. Kalyanapuram, C. Langer and K. Patatoukos,Prescriptive unitarity with elliptic leading singularities,Phys. Rev. D104(2021) 125009 [2102.02210]

  54. [54]

    C. Duhr, F. Porkert, C. Semper and S.F. Stawinski,Self-duality from twisted cohomology, JHEP03(2025) 053 [2408.04904]

  55. [55]

    C. Duhr, S. Maggio, F. Porkert, C. Semper, Y. Sohnle and S.F. Stawinski,Canonical differential equations and intersection matrices,JHEP02(2026) 211 [2509.17787]

  56. [56]

    Brown and A

    F.C.S. Brown and A. Levin,Multiple Elliptic Polylogarithms,1110.6917

  57. [57]

    Mastrolia and S

    P. Mastrolia and S. Mizera,Feynman Integrals and Intersection Theory,JHEP02(2019) 139 [1810.03818]

  58. [58]

    Mizera,Scattering Amplitudes from Intersection Theory,Phys

    S. Mizera,Scattering Amplitudes from Intersection Theory,Phys. Rev. Lett.120(2018) 141602 [1711.00469]

  59. [59]

    Bargiela, H

    P. Bargiela, H. Frellesvig, R. Marzucca, R. Morales, F. Seefeld, M. Wilhelm et al.,The spectrum of Feynman-integral geometries at two loops,2512.13794

  60. [60]

    Griffiths and J

    P. Griffiths and J. Harris,Principles of Algebraic Geometry, Wiley (1978)

  61. [61]

    Vanhove,The physics and the mixed Hodge structure of Feynman integrals,Proc

    P. Vanhove,The physics and the mixed Hodge structure of Feynman integrals,Proc. Symp. Pure Math.88(2014) 161 [1401.6438]

  62. [62]

    Bönisch, C

    K. Bönisch, C. Duhr, F. Fischbach, A. Klemm and C. Nega,Feynman integrals in dimensional regularization and extensions of Calabi-Yau motives,JHEP09(2022) 156 [2108.05310]

  63. [63]

    Chen,Iterated path integrals,Bull

    K.T. Chen,Iterated path integrals,Bull. Amer. Math. Soc.83(1977) 831

  64. [64]

    Broedel, C

    J. Broedel, C. Duhr, F. Dulat, B. Penante and L. Tancredi,Elliptic Feynman integrals and pure functions,JHEP01(2019) 023 [1809.10698]

  65. [65]

    Primo and L

    A. Primo and L. Tancredi,On the maximal cut of Feynman integrals and the solution of their differential equations,Nucl. Phys. B916(2017) 94 [1610.08397]

  66. [66]

    Primo and L

    A. Primo and L. Tancredi,Maximal cuts and differential equations for Feynman integrals. An application to the three-loop massive banana graph,Nucl. Phys. B921(2017) 316 [1704.05465]

  67. [67]

    Frellesvig and C.G

    H. Frellesvig and C.G. Papadopoulos,Cuts of Feynman Integrals in Baikov representation, JHEP04(2017) 083 [1701.07356]

  68. [68]

    Bosma, M

    J. Bosma, M. Sogaard and Y. Zhang,Maximal Cuts in Arbitrary Dimension,JHEP08 (2017) 051 [1704.04255]. – 47 –

  69. [69]

    Broedel, C

    J. Broedel, C. Duhr, F. Dulat and L. Tancredi,Elliptic polylogarithms and iterated integrals on elliptic curves. Part I: general formalism,JHEP05(2018) 093 [1712.07089]

  70. [70]

    Frellesvig,The Loop-by-Loop Baikov Representation – Strategies and Implementation, 2412.01804

    H. Frellesvig,The Loop-by-Loop Baikov Representation – Strategies and Implementation, 2412.01804

  71. [71]

    Studerus,Reduze – Feynman integral reduction in C++,Comput

    C. Studerus,Reduze – Feynman integral reduction in C++,Comput. Phys. Commun.181 (2010) 1293 [0912.2546]

  72. [72]

    von Manteuffel and C

    A. von Manteuffel and C. Studerus,Top quark pairs at two loops and Reduze 2,PoSLL2012 (2012) 059 [1210.1436]. – 48 –