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arxiv: 2606.28052 · v1 · pith:HY35DYO6new · submitted 2026-06-26 · ✦ hep-th

Planar loop integrands from cuts in D dimensions

Pith reviewed 2026-06-29 03:42 UTC · model grok-4.3

classification ✦ hep-th
keywords planar loop integrandsgeneralized unitarity cutsMöbius inversionrefinement posetD-dimensional cutscolor-ordered amplitudesYang-Mills theory
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0 comments X

The pith

A Möbius-inversion formula on the refinement poset of scalar graphs reconstructs planar loop integrands from D-dimensional cuts.

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

The paper develops a reconstruction method that builds the integrand for any L-loop n-point color-ordered planar amplitude directly from its generalized unitarity cuts taken in D dimensions. The combinatorial coefficients that combine these cuts are universal across colored theories and come from the Möbius function of a refinement poset whose elements are admissible non-scaleless scalar graphs. This separation lets the same coefficients dress theory-dependent tree amplitudes that are glued to form the cuts. The resulting expressions are written explicitly for pure Yang-Mills theory at two and three loops and become simpler in maximally supersymmetric Yang-Mills because bubble and triangle subgraphs drop out.

Core claim

For the L-loop n-point color-ordered amplitude, the planar integrand equals the sum over admissible non-scaleless scalar graphs of each graph's D-dimensional cut multiplied by the Möbius-inversion coefficient of that graph in the refinement poset, or equivalently by one minus the Euler characteristic of the associated complex.

What carries the argument

The refinement poset of admissible non-scaleless scalar graphs, whose Möbius function supplies the coefficients that assemble D-dimensional cuts into the full integrand.

If this is right

  • Closed-form integrands are obtained for two-loop five-point and six-point amplitudes in pure Yang-Mills by gluing D-dimensional tree amplitudes and summing over internal gluon states.
  • After integration-by-parts reduction the two-loop five-point result matches known integrated helicity amplitudes.
  • Compact cut-organized data are produced for the three-loop four-point case.
  • The relevant poset shrinks in maximally supersymmetric Yang-Mills because bubble and triangle subgraphs are absent.

Where Pith is reading between the lines

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

  • The same poset construction could be tested on non-planar amplitudes once a suitable definition of admissible graphs is supplied.
  • The cut-organized output may simplify numerical integration or reduction algorithms by isolating independent contributions before any integration-by-parts step.
  • The framework could be applied to amplitudes with massive particles by extending the scalar graphs to carry mass parameters inside the cuts.

Load-bearing premise

The admissible non-scaleless scalar graphs and the refinement poset they form include every contribution to the planar integrand exactly once when the D-dimensional cuts are inserted.

What would settle it

An independent calculation of the three-loop four-point pure Yang-Mills integrand that produces a result different from the explicit expression obtained by applying the Möbius formula to the admissible graphs.

read the original abstract

We present a direct reconstruction formula for planar loop integrands from $D$-dimensional generalized unitarity cuts in any colored theory. The reconstruction combinatorics is separated from the theory-dependent tree amplitudes entering the cuts: for the $L$-loop $n$-point color-ordered amplitude, the integrand is expressed as a sum over admissible non-scaleless scalar graphs dressed by corresponding cuts in $D$ dimensions; the coefficients are given by the universal M\"obius-inversion formula of the refinement poset, or equivalently one minus the Euler characteristics of associated complexes. As an application we write down closed-formulas for loop integrands in pure Yang--Mills theory, where the required cuts are generated by gluing $D$-dimensional tree amplitudes and summing over internal gluon states. We also use the two-loop five-point case as a validation, comparing with known integrand data and after integration-by-parts reduction, with known integrated helicity amplitudes. The same framework also produces compact cut-organized data for larger examples, including the two-loop six-point and three-loop four-point cases. We also describe the corresponding simplification in maximally supersymmetric Yang--Mills theory, where the absence of bubble and triangle subgraphs reduces the relevant cut poset substantially.

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 paper presents a reconstruction formula for planar L-loop n-point color-ordered integrands in any colored theory, expressing the integrand as a sum over admissible non-scaleless scalar graphs each dressed by its D-dimensional cut, with coefficients given by the universal Möbius function of the refinement poset (or equivalently 1 minus the Euler characteristic of associated complexes). The combinatorics is separated from theory-dependent tree amplitudes. Applications include closed-form expressions for pure Yang-Mills integrands via gluing of D-dimensional trees, validation on the two-loop five-point case against known integrands and integrated amplitudes, and compact cut-organized data for two-loop six-point and three-loop four-point cases, with a noted simplification in maximally supersymmetric Yang-Mills due to absence of bubble and triangle subgraphs.

Significance. If the central reconstruction holds, the result provides a theory-independent combinatorial tool for building loop integrands directly from cuts, with universal coefficients independent of the specific theory. Strengths include the explicit separation of graph combinatorics from tree amplitudes, the use of Möbius inversion on the poset, and concrete validation on the two-loop five-point case with comparison to known data after IBP reduction. The framework yields closed forms and compact expressions for higher-multiplicity cases, which could aid systematic computations in Yang-Mills and supersymmetric theories.

major comments (2)
  1. [§2] §2 (reconstruction formula): The central claim that the refinement poset of admissible non-scaleless scalar graphs is complete and that its Möbius inversion yields exact coefficients without omissions or overcounts is load-bearing. The manuscript validates this only for the two-loop five-point case; a general argument establishing that every planar contribution appears exactly once in the poset (independent of the theory-dependent trees) is needed to support the claim for arbitrary L and n.
  2. [Validation section] Validation section (two-loop five-point): While the paper states agreement with known integrand data and integrated helicity amplitudes, the explicit list of all admissible graphs, their refinement relations, and the resulting linear combination after inserting the D-dimensional cuts is not provided. This makes it impossible to verify that the Möbius coefficients precisely cancel multiple-counted lower-order cuts for even this benchmark case.
minor comments (2)
  1. Notation for the poset and admissible graphs should be defined more explicitly at first use, including a clear statement of what 'non-scaleless' excludes.
  2. The abstract mentions 'closed-formulas' for Yang-Mills but the main text should include at least one fully expanded example (e.g., a specific coefficient for a graph in the two-loop five-point case) to illustrate the Möbius function in action.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their careful reading and constructive comments. We address the two major points below. We agree that additional clarification on the generality of the poset construction would strengthen the manuscript and will revise accordingly. We also agree to expand the validation section with explicit data for the benchmark case.

read point-by-point responses
  1. Referee: [§2] §2 (reconstruction formula): The central claim that the refinement poset of admissible non-scaleless scalar graphs is complete and that its Möbius inversion yields exact coefficients without omissions or overcounts is load-bearing. The manuscript validates this only for the two-loop five-point case; a general argument establishing that every planar contribution appears exactly once in the poset (independent of the theory-dependent trees) is needed to support the claim for arbitrary L and n.

    Authors: The refinement poset is defined combinatorially on the set of all admissible non-scaleless scalar graphs that can appear in planar color-ordered amplitudes, with the partial order given by refinement of subgraphs. By construction, this set is exhaustive for planar contributions because any planar integrand can be expressed in terms of such graphs (the admissibility condition encodes planarity and the non-scaleless requirement excludes vanishing contributions). The Möbius function of this poset is universal and independent of the specific theory or the tree amplitudes that dress the cuts; it arises solely from the incidence algebra of the poset. Möbius inversion then guarantees that the linear combination exactly inverts the sum over all refinements, ensuring each planar contribution appears with coefficient 1 and no overcounts occur. This argument is theory-independent because the poset structure does not reference the internal states or the specific cut values. We will add a dedicated subsection in §2 spelling out this general combinatorial argument, including a proof that the poset is complete for planar graphs. revision: yes

  2. Referee: [Validation section] Validation section (two-loop five-point): While the paper states agreement with known integrand data and integrated helicity amplitudes, the explicit list of all admissible graphs, their refinement relations, and the resulting linear combination after inserting the D-dimensional cuts is not provided. This makes it impossible to verify that the Möbius coefficients precisely cancel multiple-counted lower-order cuts for even this benchmark case.

    Authors: We agree that the explicit enumeration would improve verifiability. The two-loop five-point case involves a modest number of admissible graphs (approximately two dozen after symmetry considerations), and the refinement relations can be listed systematically. We will add an appendix containing the complete list of admissible graphs, the Hasse diagram of the refinement poset, the Möbius coefficients for each, and the explicit linear combination of D-dimensional cuts. This will allow direct verification that lower-order cuts cancel as required by the inversion formula. The comparison to known integrand data and integrated amplitudes will remain in the main text. revision: yes

Circularity Check

0 steps flagged

No significant circularity; Möbius inversion on graph refinement poset is standard combinatorial reconstruction

full rationale

The paper presents a reconstruction of planar loop integrands as a sum over admissible non-scaleless scalar graphs with coefficients from the universal Möbius function of the refinement poset (or 1 minus Euler characteristics). This applies a standard poset-theoretic inversion to a poset defined by explicit graph inclusion/refinement relations, separating combinatorics from theory-dependent cuts. No self-definitional loops, fitted parameters renamed as predictions, or load-bearing self-citations appear; the formula is not equivalent to its inputs by construction but follows from the definition of Möbius inversion on the stated poset. The derivation remains self-contained against external combinatorial benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The reconstruction rests on the existence of a well-defined refinement poset of non-scaleless scalar graphs whose Möbius function yields the correct coefficients when multiplied by D-dimensional cuts; no free parameters or new entities are introduced in the abstract.

axioms (2)
  • domain assumption The refinement poset of admissible scalar graphs admits a Möbius function that correctly assigns coefficients to each graph contribution.
    Invoked when the abstract states that coefficients are given by the universal Möbius-inversion formula of the refinement poset.
  • domain assumption D-dimensional generalized unitarity cuts are sufficient to determine the planar integrand once the combinatorial coefficients are known.
    Stated in the opening sentence as the basis for the direct reconstruction formula.

pith-pipeline@v0.9.1-grok · 5748 in / 1553 out tokens · 39257 ms · 2026-06-29T03:42:47.693278+00:00 · methodology

discussion (0)

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Reference graph

Works this paper leans on

71 extracted references · 43 linked inside Pith

  1. [1]

    Elvang and Y.-t

    H. Elvang and Y.-t. Huang,Scattering Amplitudes in Gauge Theory and Gravity. Cambridge University Press, 2015

  2. [2]

    Arkani-Hamed, Y

    N. Arkani-Hamed, Y. Bai, S. He, and G. Yan,Scattering Forms and the Positive Geometry of Kinematics, Color and the Worldsheet,JHEP05(2018) 096, [arXiv:1711.09102]

  3. [3]

    Herrmann and J

    E. Herrmann and J. Trnka,The SAGEX review on scattering amplitudes Chapter 7: Positive geometry of scattering amplitudes,J. Phys. A55(2022), no. 44 443008, [arXiv:2203.13018]

  4. [4]

    Z. Bern, J. J. M. Carrasco, and H. Johansson,New Relations for Gauge-Theory Amplitudes, Phys. Rev. D78(2008) 085011, [arXiv:0805.3993]

  5. [5]

    Z. Bern, J. J. M. Carrasco, and H. Johansson,Perturbative Quantum Gravity as a Double Copy of Gauge Theory,Phys. Rev. Lett.105(2010) 061602, [arXiv:1004.0476]

  6. [6]

    Z. Bern, J. J. M. Carrasco, L. J. Dixon, H. Johansson, and R. Roiban,Simplifying Multiloop Integrands and Ultraviolet Divergences of Gauge Theory and Gravity Amplitudes,Phys. Rev. D85(2012) 105014, [arXiv:1201.5366]

  7. [7]

    Z. Bern, S. Davies, and J. Nohle,Double-Copy Constructions and Unitarity Cuts,Phys. Rev. D93(2016), no. 10 105015, [arXiv:1510.03448]

  8. [8]

    Z. Bern, J. J. Carrasco, W.-M. Chen, A. Edison, H. Johansson, J. Parra-Martinez, R. Roiban, and M. Zeng,Ultraviolet Properties ofN= 8Supergravity at Five Loops,Phys. Rev. D98(2018), no. 8 086021, [arXiv:1804.09311]

  9. [9]

    Z. Bern, J. J. Carrasco, M. Chiodaroli, H. Johansson, and R. Roiban,The duality between color and kinematics and its applications,J. Phys. A57(2024), no. 33 333002, [arXiv:1909.01358]

  10. [10]

    Cachazo, S

    F. Cachazo, S. He, and E. Y. Yuan,Scattering of Massless Particles in Arbitrary Dimensions,Phys. Rev. Lett.113(2014), no. 17 171601, [arXiv:1307.2199]

  11. [11]

    Cachazo, S

    F. Cachazo, S. He, and E. Y. Yuan,Scattering of Massless Particles: Scalars, Gluons and Gravitons,JHEP07(2014) 033, [arXiv:1309.0885]

  12. [12]

    Cachazo, S

    F. Cachazo, S. He, and E. Y. Yuan,Scattering Equations and Matrices: From Einstein To Yang-Mills, DBI and NLSM,JHEP07(2015) 149, [arXiv:1412.3479]

  13. [13]

    Arkani-Hamed, H

    N. Arkani-Hamed, H. Frost, G. Salvatori, P.-G. Plamondon, and H. Thomas,All loop scattering as a counting problem,JHEP08(2025) 194, [arXiv:2309.15913]

  14. [14]

    Arkani-Hamed, H

    N. Arkani-Hamed, H. Frost, G. Salvatori, P.-G. Plamondon, and H. Thomas,All loop scattering for all multiplicity,JHEP09(2025) 033, [arXiv:2311.09284]

  15. [15]

    Arkani-Hamed, Q

    N. Arkani-Hamed, Q. Cao, J. Dong, C. Figueiredo, and S. He,Hidden zeros for particle/string amplitudes and the unity of colored scalars, pions and gluons,JHEP10 (2024) 231, [arXiv:2312.16282]

  16. [16]

    He and C

    S. He and C. Zhang,Notes on Scattering Amplitudes as Differential Forms,JHEP10(2018) 054, [arXiv:1807.11051]

  17. [17]

    R. E. Cutkosky,Singularities and discontinuities of feynman amplitudes,J. Math. Phys.1 (1960) 429–433

  18. [18]

    Z. Bern, L. Dixon, D. C. Dunbar, and D. A. Kosower,One-loop n-point gauge theory 23 amplitudes, unitarity and collinear limits,Nucl. Phys. B425(1994) 217–260, [hep-ph/9403226]

  19. [19]

    Z. Bern, L. J. Dixon, D. C. Dunbar, and D. A. Kosower,Fusing gauge theory tree amplitudes into loop amplitudes,Nucl. Phys. B435(1995) 59–101, [hep-ph/9409265]

  20. [20]

    Britto, F

    R. Britto, F. Cachazo, and B. Feng,Generalized unitarity and one-loop amplitudes in n=4 super-yang-mills,Nucl. Phys. B725(2005) 275–305, [hep-th/0412103]

  21. [21]

    Bern and Y.-t

    Z. Bern and Y.-t. Huang,Basics of generalized unitarity,arXiv:1103.1869

  22. [22]

    Bern and A

    Z. Bern and A. G. Morgan,Massive loop amplitudes from unitarity,hep-ph/9511336

  23. [23]

    Forde,Direct extraction of one-loop integral coefficients,arXiv:0704.1835

    D. Forde,Direct extraction of one-loop integral coefficients,arXiv:0704.1835

  24. [24]

    D. A. Kosower and K. J. Larsen,Maximal unitarity at two loops,Phys. Rev. D85(2012) 045017, [arXiv:1108.1180]

  25. [25]

    Abreu, F

    S. Abreu, F. Febres Cordero, H. Ita, M. Jaquier, and B. Page,Subleading poles in the numerical unitarity method at two loops,Phys. Rev. D95(2017) 096011, [arXiv:1703.05255]

  26. [26]

    Brandhuber, S

    A. Brandhuber, S. McNamara, B. Spence, and G. Travaglini,Loop amplitudes in pure yang-mills from generalised unitarity,JHEP10(2005) 011, [hep-th/0506068]

  27. [27]

    Badger, G

    S. Badger, G. Mogull, A. Ochirov, and D. O’Connell,A Complete Two-Loop, Five-Gluon Helicity Amplitude in Yang-Mills Theory,JHEP10(2015) 064, [arXiv:1507.08797]

  28. [28]

    D. C. Dunbar, G. R. Jehu, and W. B. Perkins,The two-loop n-point all-plus helicity amplitude,Phys. Rev. D93(2016), no. 12 125006, [arXiv:1604.06631]

  29. [29]

    Badger, G

    S. Badger, G. Mogull, and T. Peraro,Local integrands for two-loop all-plus Yang-Mills amplitudes,JHEP08(2016) 063, [arXiv:1606.02244]

  30. [30]

    Abreu, F

    S. Abreu, F. Febres Cordero, H. Ita, B. Page, and M. Zeng,Planar two-loop five-gluon amplitudes from numerical unitarity,arXiv:1712.03946

  31. [31]

    Badger, C

    S. Badger, C. Brønnum-Hansen, H. B. Hartanto, and T. Peraro,First look at two-loop five-gluon scattering in QCD,Phys. Rev. Lett.120(2018), no. 9 092001, [arXiv:1712.02229]

  32. [32]

    Abreu, F

    S. Abreu, F. Febres Cordero, H. Ita, B. Page, and V. Sotnikov,Planar Two-Loop Five-Parton Amplitudes from Numerical Unitarity,JHEP11(2018) 116, [arXiv:1809.09067]

  33. [33]

    Abreu, J

    S. Abreu, J. Dormans, F. Febres Cordero, H. Ita, and B. Page,Analytic Form of Planar Two-Loop Five-Gluon Scattering Amplitudes in QCD,Phys. Rev. Lett.122(2019), no. 8 082002, [arXiv:1812.04586]

  34. [34]

    Abreu, J

    S. Abreu, J. Dormans, F. Febres Cordero, H. Ita, B. Page, and V. Sotnikov,Analytic Form of the Planar Two-Loop Five-Parton Scattering Amplitudes in QCD,JHEP05(2019) 084, [arXiv:1904.00945]

  35. [35]

    D. C. Dunbar, W. B. Perkins, and J. M. W. Strong,n-point QCD two-loop amplitude,Phys. Rev. D101(2020), no. 7 076001, [arXiv:2001.11347]

  36. [36]

    Jin and H

    Q. Jin and H. Luo,Analytic form of the three-loop four-gluon scattering amplitudes in yang-mills theory,arXiv:1910.05889

  37. [37]

    D. A. Kosower and S. P¨ ogel,A Unitarity Approach to Two-Loop All-Plus Rational Terms, arXiv:2206.14445. 24

  38. [38]

    Carrˆ olo, D

    S. Carrˆ olo, D. Chicherin, J. Henn, Q. Yang, and Y. Zhang,Qcd scattering amplitudes and prescriptive unitarity,arXiv:2602.02783

  39. [39]

    J. L. Bourjaily, E. Herrmann, and J. Trnka,Prescriptive unitarity,arXiv:1704.05460

  40. [40]

    J. L. Bourjaily, E. Herrmann, C. Langer, A. J. McLeod, and J. Trnka,Prescriptive Unitarity for Non-Planar Six-Particle Amplitudes at Two Loops,JHEP12(2019) 073, [arXiv:1909.09131]

  41. [41]

    J. L. Bourjaily, E. Herrmann, C. Langer, A. J. McLeod, and J. Trnka,All-Multiplicity Nonplanar Amplitude Integrands in Maximally Supersymmetric Yang-Mills Theory at Two Loops,Phys. Rev. Lett.124(2020), no. 11 111603, [arXiv:1911.09106]

  42. [42]

    J. L. Bourjaily, E. Herrmann, C. Langer, and J. Trnka,Building bases of loop integrands, JHEP11(2020) 116, [arXiv:2007.13905]

  43. [43]

    J. L. Bourjaily, N. Kalyanapuram, C. Langer, and K. Patatoukos,Prescriptive unitarity with elliptic leading singularities,Phys. Rev. D104(2021), no. 12 125009, [arXiv:2102.02210]

  44. [44]

    J. L. Bourjaily, E. Herrmann, C. Langer, K. Patatoukos, J. Trnka, and M. Zheng,Integrands of less-supersymmetric Yang-Mills at one loop,JHEP03(2022) 126, [arXiv:2112.06901]

  45. [45]

    J. L. Bourjaily, C. Langer, and Y. Zhang,Illustrations of integrand-basis building at two loops,JHEP08(2022) 176, [arXiv:2112.05157]

  46. [46]

    Zhang,Integrand-level reduction of loop amplitudes by computational algebraic geometry methods,arXiv:1205.5707

    Y. Zhang,Integrand-level reduction of loop amplitudes by computational algebraic geometry methods,arXiv:1205.5707

  47. [47]

    Mastrolia, E

    P. Mastrolia, E. Mirabella, G. Ossola, and T. Peraro,Scattering Amplitudes from Multivariate Polynomial Division,Phys. Lett. B718(2012) 173–177, [arXiv:1205.7087]

  48. [48]

    Mastrolia, E

    P. Mastrolia, E. Mirabella, G. Ossola, and T. Peraro,Integrand reduction for two-loop scattering amplitudes through multivariate polynomial division,arXiv:1209.4319

  49. [49]

    Ita,Two-loop integrand decomposition into master integrals and surface terms, arXiv:1510.05626

    H. Ita,Two-loop integrand decomposition into master integrals and surface terms, arXiv:1510.05626

  50. [50]

    Arkani-Hamed, Q

    N. Arkani-Hamed, Q. Cao, J. Dong, C. Figueiredo, and S. He,Surface Kinematics and the Canonical Yang-Mills All-Loop Integrand,Phys. Rev. Lett.134(2025) 171601, [arXiv:2408.11891]

  51. [51]

    Cao and F

    Q. Cao and F. Zhu,All-loop planar integrands in Yang-Mills theory from recursion,Phys. Rev. D112(2025), no. 8 085012, [arXiv:2503.15860]

  52. [52]

    Ossola, C

    G. Ossola, C. G. Papadopoulos, and R. Pittau,Reducing full one-loop amplitudes to scalar integrals at the integrand level,Nucl. Phys. B763(2007) 147–169, [hep-ph/0609007]

  53. [53]

    Arkani-Hamed, Q

    N. Arkani-Hamed, Q. Cao, J. Dong, C. Figueiredo, and S. He,Scalar-scaffolded gluons and the combinatorial origins of Yang-Mills theory,JHEP04(2025) 078, [arXiv:2401.00041]

  54. [54]

    Arkani-Hamed, Q

    N. Arkani-Hamed, Q. Cao, J. Dong, C. Figueiredo, and S. He,Nonlinear Sigma model amplitudes to all loop orders are contained in the Tr(Φ 3) theory,Phys. Rev. D110(2024), no. 6 065018, [arXiv:2401.05483]

  55. [55]

    Arkani-Hamed, C

    N. Arkani-Hamed, C. Figueiredo, H. Frost, and G. Salvatori,Tropical amplitudes for colored Lagrangians,JHEP05(2025) 051, [arXiv:2402.06719]

  56. [56]

    Arkani-Hamed and C

    N. Arkani-Hamed and C. Figueiredo,Circles and triangles, the NLSM and Tr(Φ 3),JHEP09 (2025) 189, [arXiv:2403.04826]. 25

  57. [57]

    S. De, A. Pokraka, M. Skowronek, M. Spradlin, and A. Volovich,Surfaceology for colored Yukawa theory,JHEP09(2024) 160, [arXiv:2406.04411]

  58. [58]

    Arkani-Hamed, H

    N. Arkani-Hamed, H. Frost, and G. Salvatori,The Cut Equation,arXiv:2412.21027

  59. [59]

    Q. Cao, J. Dong, S. He, and F. Zhu,One-loop amplitudes in gauge theories,Phys. Rev. D 111(2025), no. 6 065015, [arXiv:2412.19629]

  60. [60]

    Rota,On the foundations of combinatorial theory i

    G.-C. Rota,On the foundations of combinatorial theory i. theory of m¨ obius functions,Z. Wahrscheinlichkeitstheorie verw. Gebiete2(1964) 340–368

  61. [61]

    Z. Bern, E. Herrmann, S. Litsey, J. Stankowicz, and J. Trnka,Logarithmic Singularities and Maximally Supersymmetric Amplitudes,JHEP06(2015) 202, [arXiv:1412.8584]

  62. [62]

    Ochirov and B

    A. Ochirov and B. Page,Full Colour for Loop Amplitudes in Yang-Mills Theory,JHEP02 (2017) 100, [arXiv:1612.04366]

  63. [63]

    Edison, S

    A. Edison, S. He, O. Schlotterer, and F. Teng,One-loop Correlators and BCJ Numerators from Forward Limits,JHEP09(2020) 079, [arXiv:2005.03639]

  64. [64]

    Z. Bern, A. De Freitas, and L. J. Dixon,Two loop helicity amplitudes for gluon-gluon scattering in QCD and supersymmetric Yang-Mills theory,JHEP03(2002) 018, [hep-ph/0201161]

  65. [65]

    C. R. Mafra, O. Schlotterer, S. Stieberger, and D. Tsimpis,A recursive method for SYM n-point tree amplitudes,Phys. Rev. D83(2011) 126012, [arXiv:1012.3981]

  66. [66]

    C. R. Mafra and O. Schlotterer,Multiparticle SYM equations of motion and pure spinor BRST blocks,JHEP07(2014) 153, [arXiv:1404.4986]

  67. [67]

    C. R. Mafra and O. Schlotterer,Berends-Giele Recursions and the BCJ Duality in Superspace and Components,JHEP03(2016) 097, [arXiv:1510.08846]

  68. [68]

    Edison, S

    A. Edison, S. He, H. Johansson, O. Schlotterer, F. Teng, and Y. Zhang,Perfecting one-loop BCJ numerators in SYM and supergravity,JHEP02(2023) 164, [arXiv:2211.00638]

  69. [69]

    Del Duca, L

    V. Del Duca, L. J. Dixon, and F. Maltoni,New color decompositions for gauge amplitudes at tree and loop level,Nucl. Phys. B571(2000) 51–70, [hep-ph/9910563]

  70. [70]

    Z. Bern, E. Herrmann, R. Roiban, M. S. Ruf, and M. Zeng,Global bases for nonplanar loop integrands, generalized unitarity, and the double copy to all loop orders,arXiv:2408.06686

  71. [71]

    Cachazo, S

    F. Cachazo, S. He, and E. Y. Yuan,Einstein-Yang-Mills Scattering Amplitudes From Scattering Equations,JHEP01(2015) 121, [arXiv:1409.8256]. 26