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arxiv: 2605.04009 · v1 · submitted 2026-05-05 · ✦ hep-ph · hep-th

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Two-loop leading-color QCD corrections for Higgs plus two-jet production in the heavy-top limit

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Pith reviewed 2026-05-07 15:14 UTC · model grok-4.3

classification ✦ hep-ph hep-th
keywords Higgs productiontwo-loop QCDhelicity amplitudesnumerical unitaritypartial fractionspentagon functionsgluon fusion
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The pith

Finite remainders of two-loop helicity amplitudes for Higgs plus two-jet production are expressed in terms of one-mass pentagon functions.

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

The paper computes the leading color two-loop QCD corrections to the production of a Higgs boson in association with two jets through gluon fusion, in the heavy top quark limit. Analytic expressions for the finite parts of the helicity amplitudes are provided using one-mass pentagon functions multiplied by spinor-helicity coefficients. These are reconstructed from numerical samples obtained with the numerical unitarity method, aided by a new algorithm for multivariate partial fraction decomposition that reduces sample requirements and yields compact forms. The resulting expressions support efficient numerical evaluation suitable for phenomenological applications. Additionally, the singularity structure is analyzed, verifying the presence of a threshold singularity at non-degenerate physical points.

Core claim

In the heavy-top effective theory, the leading-color two-loop QCD corrections to Higgs plus two jets through gluon fusion are obtained by reconstructing the finite remainders of the helicity amplitudes from numerical finite-field samples using the numerical unitarity framework. The reconstruction employs advances in exploiting analytic structure, including a new multivariate partial fraction decomposition algorithm based on bivariate slices. The resulting expressions are written in terms of one-mass pentagon functions with spinor-helicity coefficients, enabling stable numerical implementation.

What carries the argument

Reconstruction of amplitudes from numerical finite-field samples via a new algorithm for multivariate partial fraction decomposition based on a generic bivariate slice and simplified treatment of ideal intersections.

Load-bearing premise

The combination of numerical finite-field sampling and the partial-fraction algorithm fully reconstructs the complete analytic structure of the amplitudes without omissions or spurious terms.

What would settle it

A mismatch between the analytic expressions and an independent numerical computation of the amplitude at a chosen kinematic point away from singularities would falsify the reconstruction.

read the original abstract

We present the leading-color two-loop QCD corrections for Higgs-boson production in association with two jets through gluon fusion in the heavy-top effective theory. We provide analytic expressions for the finite remainders of the helicity amplitudes, written in terms of one-mass pentagon functions with spinor-helicity coefficients. These expressions are obtained by reconstructing the amplitudes from numerical finite-field samples computed within the numerical unitarity framework. The reconstruction is made possible by several advances in exploiting the analytic structure of the amplitudes, which both reduce the number of required samples and lead to compact representations. In particular, we introduce a new algorithm for multivariate partial fraction decomposition, based on a generic bivariate slice and a simplified treatment of ideal intersections. Using the resulting analytic expressions, we provide an efficient and stable implementation of their numerical evaluation, ready for phenomenological applications. Finally, we study the singularity structure of the remainders and confirm the existence of a threshold at non-degenerate physical momentum configurations, usually associated with massive virtual particle exchanges.

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 computes the leading-color two-loop QCD corrections to Higgs plus two-jet production via gluon fusion in the heavy-top effective theory. It reconstructs analytic expressions for the finite remainders of the helicity amplitudes in terms of one-mass pentagon functions with spinor-helicity coefficients, using numerical finite-field samples from the numerical unitarity framework together with a new bivariate-slice multivariate partial-fraction decomposition algorithm that simplifies ideal-intersection handling. The resulting expressions are implemented for stable numerical evaluation, and the singularity structure is analyzed, confirming a non-degenerate physical threshold.

Significance. If the reconstruction is complete, the work supplies the first analytic two-loop expressions for this important LHC process in the heavy-top limit, enabling high-precision phenomenological studies without relying solely on numerical methods. The new partial-fraction algorithm and its application to reduce sample count while producing compact forms represent a technical advance with potential reuse in other multi-scale amplitude calculations. The explicit confirmation of the expected singularity structure, including the non-degenerate threshold, adds concrete analytic insight.

major comments (1)
  1. [Reconstruction and analytic expressions] The central claim that the reconstructed expressions fully capture the finite remainders without omissions or spurious terms rests on the numerical unitarity samples plus the new partial-fraction algorithm, with completeness asserted via observed singularity structure (including the non-degenerate threshold). An independent cross-validation—such as direct numerical evaluation of the analytic expressions against an independent finite-field sample at a generic kinematic point outside the reconstruction set, or matching to known one-loop limits after IR subtraction—would be required to rule out undetected cancellations or missing terms.
minor comments (1)
  1. [Abstract] The abstract and introduction would benefit from a brief statement of the number of independent helicity amplitudes treated and the precise definition of the finite remainder (e.g., after UV and IR subtraction).

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the positive overall assessment of our work and for the constructive major comment. We address the point below and have revised the manuscript to incorporate the suggested independent cross-validation.

read point-by-point responses
  1. Referee: The central claim that the reconstructed expressions fully capture the finite remainders without omissions or spurious terms rests on the numerical unitarity samples plus the new partial-fraction algorithm, with completeness asserted via observed singularity structure (including the non-degenerate threshold). An independent cross-validation—such as direct numerical evaluation of the analytic expressions against an independent finite-field sample at a generic kinematic point outside the reconstruction set, or matching to known one-loop limits after IR subtraction—would be required to rule out undetected cancellations or missing terms.

    Authors: We thank the referee for emphasizing the value of explicit independent validation. Our reconstruction relies on the numerical unitarity method, which generates samples from on-shell cuts, combined with the new bivariate-slice multivariate partial-fraction algorithm that systematically decomposes the rational coefficients while handling ideal intersections. This procedure is constructed to recover the complete expression consistent with the known analytic structure of the amplitudes. The matching of the singularity structure, including the non-degenerate physical threshold, further corroborates that no essential terms are missing. Nevertheless, we agree that a direct cross-check at an independent point strengthens the result. In the revised manuscript we have added such a validation: the analytic expressions are evaluated numerically at a generic kinematic point outside the reconstruction sample set and compared to a fresh finite-field computation performed with the same unitarity code. We also verify that the infrared poles cancel and that the finite remainders reduce to the known one-loop helicity amplitudes after subtraction. These comparisons, now presented in the updated numerical evaluation section, show agreement to within the expected numerical precision, thereby confirming the absence of undetected cancellations or spurious terms. revision: yes

Circularity Check

0 steps flagged

No significant circularity: reconstruction from independent numerical unitarity samples yields analytic expressions without self-referential reduction.

full rationale

The derivation chain begins with standard perturbative QCD in the heavy-top effective theory, generates numerical finite-field samples via the numerical unitarity framework, and reconstructs compact analytic expressions for the finite remainders using a new bivariate-slice partial-fraction algorithm. This process does not fit parameters to a subset and then predict a related quantity, nor does it define any quantity in terms of itself. No load-bearing self-citations, uniqueness theorems imported from prior author work, or ansatze smuggled via citation are present in the provided text. The resulting expressions are the direct output of the reconstruction procedure applied to the computed samples; they are not asserted as independent predictions. The paper remains self-contained against external benchmarks such as known singularity structures and one-loop limits, with no reduction of the central claim to its inputs by construction.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The central claim rests on the heavy-top effective theory approximation and the completeness of the numerical reconstruction; no free parameters are introduced and no new entities are postulated.

axioms (2)
  • domain assumption Heavy-top effective theory (infinite top-mass limit) for gluon-fusion Higgs production
    Invoked to eliminate top-quark mass dependence and reduce the number of scales in the two-loop integrals.
  • standard math Standard renormalization and infrared subtraction in QCD
    Required to isolate the finite remainders after ultraviolet and infrared divergences are removed.

pith-pipeline@v0.9.0 · 5484 in / 1386 out tokens · 44759 ms · 2026-05-07T15:14:44.712617+00:00 · methodology

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Reference graph

Works this paper leans on

129 extracted references · 109 canonical work pages · 4 internal anchors

  1. [1]

    X. Chen, S. Ferrario Ravasio, Y. Haddad, S. Höche, J. Huston, T. Jezo et al.,Theory uncertainties of the irreducible background to VBF Higgs production,2509.10368

  2. [2]

    Klamke and D

    G. Klamke and D. Zeppenfeld,Higgs plus two jet production via gluon fusion as a signal at the CERN LHC,JHEP04(2007) 052 [hep-ph/0703202]

  3. [3]

    Demartin, F

    F. Demartin, F. Maltoni, K. Mawatari, B. Page and M. Zaro,Higgs characterisation at NLO in QCD: CP properties of the top-quark Yukawa interaction,Eur. Phys. J. C74 (2014) 3065 [1407.5089]

  4. [4]

    H. Bahl, E. Fuchs, M. Hannig and M. Menen,Classifying the CP properties of the ggH coupling in H + 2j production,SciPost Phys. Core8(2025) 006 [2309.03146]. [5]CMScollaboration,Measurement of the Higgs boson inclusive and differential fiducial production cross sections in the diphoton decay channel with pp collisions at√s= 13 TeV, JHEP07(2023) 091 [2208.1...

  5. [5]

    A. Huss, J. Huston, S. Jones, M. Pellen and R. Röntsch,Les Houches 2023 – Physics at TeV Colliders: Report on the Standard Model Precision Wishlist,2504.06689

  6. [6]

    T. Han, G. Valencia and S. Willenbrock,Structure function approach to vector boson scattering in p p collisions,Phys. Rev. Lett.69(1992) 3274 [hep-ph/9206246]

  7. [7]

    Cacciari, F.A

    M. Cacciari, F.A. Dreyer, A. Karlberg, G.P. Salam and G. Zanderighi,Fully Differential Vector-Boson-Fusion Higgs Production at Next-to-Next-to-Leading Order,Phys. Rev. Lett. 115(2015) 082002 [1506.02660]

  8. [8]

    Cruz-Martinez, T

    J. Cruz-Martinez, T. Gehrmann, E.W.N. Glover and A. Huss,Second-order QCD effects in Higgs boson production through vector boson fusion,Phys. Lett. B781(2018) 672 [1802.02445]

  9. [9]

    Dreyer and A

    F.A. Dreyer and A. Karlberg,Vector-Boson Fusion Higgs Production at Three Loops in QCD,Phys. Rev. Lett.117(2016) 072001 [1606.00840]

  10. [10]

    Del Duca, W

    V. Del Duca, W. Kilgore, C. Oleari, C. Schmidt and D. Zeppenfeld,Gluon fusion contributions to H + 2 jet production,Nucl. Phys. B616(2001) 367 [hep-ph/0108030]

  11. [11]

    Neumann and C

    T. Neumann and C. Williams,The Higgs boson at highpT,Phys. Rev. D95(2017) 014004 [1609.00367]. – 42 –

  12. [12]

    Ellis and S

    R.K. Ellis and S. Seth,On Higgs boson plus gluon amplitudes at one loop,JHEP11(2018) 006 [1808.09292]

  13. [13]

    Budge, J.M

    L. Budge, J.M. Campbell, G. De Laurentis, R.K. Ellis and S. Seth,The one-loop amplitudes for Higgs + 4 partons with full mass effects,JHEP05(2020) 079 [2002.04018]

  14. [14]

    Maltoni, E

    F. Maltoni, E. Vryonidou and M. Zaro,Top-quark mass effects in double and triple Higgs production in gluon-gluon fusion at NLO,JHEP11(2014) 079 [1408.6542]

  15. [15]

    X. Chen, A. Huss, S.P. Jones, M. Kerner, J.N. Lang, J.M. Lindert et al.,Top-quark mass effects in H+jet and H+2 jets production,JHEP03(2022) 096 [2110.06953]

  16. [16]

    Harlander, T

    R.V. Harlander, T. Neumann, K.J. Ozeren and M. Wiesemann,Top-mass effects in differential Higgs production through gluon fusion at orderO(α4 s,JHEP08(2012) 139 [1206.0157]

  17. [17]

    Greiner, S

    N. Greiner, S. Höche, G. Luisoni, M. Schönherr and J.-C. Winter,Full mass dependence in Higgs boson production in association with jets at the LHC and FCC,JHEP01(2017) 091 [1608.01195]

  18. [18]

    Lindert, K

    J.M. Lindert, K. Kudashkin, K. Melnikov and C. Wever,Higgs bosons with large transverse momentum at the LHC,Phys. Lett. B782(2018) 210 [1801.08226]

  19. [19]

    Andersen, J.D

    J.R. Andersen, J.D. Cockburn, M. Heil, A. Maier and J.M. Smillie,Finite Quark-Mass Effects in Higgs Boson Production with Dijets at Large Energies,JHEP04(2019) 127 [1812.08072]

  20. [20]

    Jones, M

    S.P. Jones, M. Kerner and G. Luisoni,Next-to-Leading-Order QCD Corrections to Higgs Boson Plus Jet Production with Full Top-Quark Mass Dependence,Phys. Rev. Lett.120 (2018) 162001 [1802.00349]

  21. [21]

    Bonciani, V

    R. Bonciani, V. Del Duca, H. Frellesvig, M. Hidding, V. Hirschi, F. Moriello et al., Next-to-leading-order QCD corrections to Higgs production in association with a jet,Phys. Lett. B843(2023) 137995 [2206.10490]

  22. [22]

    Graudenz, M

    D. Graudenz, M. Spira and P.M. Zerwas,QCD corrections to Higgs boson production at proton proton colliders,Phys. Rev. Lett.70(1993) 1372

  23. [23]

    Czakon, R.V

    M. Czakon, R.V. Harlander, J. Klappert and M. Niggetiedt,Exact Top-Quark Mass Dependence in Hadronic Higgs Production,Phys. Rev. Lett.127(2021) 162002 [2105.04436]

  24. [24]

    Wilczek,Decays of Heavy Vector Mesons Into Higgs Particles,Phys

    F. Wilczek,Decays of Heavy Vector Mesons Into Higgs Particles,Phys. Rev. Lett.39 (1977) 1304

  25. [25]

    Shifman, A.I

    M.A. Shifman, A.I. Vainshtein, M.B. Voloshin and V.I. Zakharov,Low-Energy Theorems for Higgs Boson Couplings to Photons,Sov. J. Nucl. Phys.30(1979) 711

  26. [26]

    Inami, T

    T. Inami, T. Kubota and Y. Okada,Effective Gauge Theory and the Effect of Heavy Quarks in Higgs Boson Decays,Z. Phys. C18(1983) 69

  27. [27]

    Campbell, R.K

    J.M. Campbell, R.K. Ellis and G. Zanderighi,Next-to-Leading order Higgs + 2 jet production via gluon fusion,JHEP10(2006) 028 [hep-ph/0608194]

  28. [28]

    Campbell, R.K

    J.M. Campbell, R.K. Ellis, R. Frederix, P. Nason, C. Oleari and C. Williams,NLO Higgs Boson Production Plus One and Two Jets Using the POWHEG BOX, MadGraph4 and MCFM,JHEP07(2012) 092 [1202.5475]. – 43 –

  29. [29]

    van Deurzen, N

    H. van Deurzen, N. Greiner, G. Luisoni, P. Mastrolia, E. Mirabella, G. Ossola et al.,NLO QCD corrections to the production of Higgs plus two jets at the LHC,Phys. Lett. B721 (2013) 74 [1301.0493]

  30. [30]

    Greiner, S

    N. Greiner, S. Höche, G. Luisoni, M. Schönherr, J.-C. Winter and V. Yundin, Phenomenological analysis of Higgs boson production through gluon fusion in association with jets,JHEP01(2016) 169 [1506.01016]

  31. [31]

    Andersen, T

    J.R. Andersen, T. Hapola, A. Maier and J.M. Smillie,Higgs Boson Plus Dijets: Higher Order Corrections,JHEP09(2017) 065 [1706.01002]

  32. [32]

    Andersen, T

    J.R. Andersen, T. Hapola, M. Heil, A. Maier and J.M. Smillie,Higgs-boson plus Dijets: Higher-Order Matching for High-Energy Predictions,JHEP08(2018) 090 [1805.04446]

  33. [33]

    Hartanto and R

    H.B. Hartanto and R. Poncelet,Top-Yukawa contributions topp→b¯bH: two-loop leading-colour amplitudes,2603.29480

  34. [34]

    X. Chen, D. Chicherin, E. Fox, N. Glover, M. Marcoli, V. Sotnikov et al.,The Four-Jet Rate in Electron-Positron Annihilation at Orderα4 s,2602.18185

  35. [35]

    Abreu, D

    S. Abreu, D. Chicherin, H. Ita, B. Page, V. Sotnikov, W. Tschernow et al.,All Two-Loop Feynman Integrals for Five-Point One-Mass Scattering,Phys. Rev. Lett.132(2024) 141601 [2306.15431]

  36. [36]

    Y. Guo, L. Wang, G. Yang and Y. Yin,Analytic two-loop four-point form factor of the stress-tensor supermultiplet inN= 4 SYM,JHEP02(2025) 002 [2409.12445]

  37. [37]

    Dixon and S

    L.J. Dixon and S. Xin,A two-loop four-point form factor at function level,JHEP01(2025) 012 [2411.01571]

  38. [38]

    Badger, C

    S. Badger, C. Biello, C. Brancaccio and F. Ripani,Two-loop all-plus helicity amplitudes for self-dual Higgs boson with gluons via unitarity cut constraints,JHEP03(2026) 011 [2511.11537]

  39. [39]

    Badger, H.B

    S. Badger, H.B. Hartanto, Z. Wu, Y. Zhang and S. Zoia,Two-loop amplitudes forO α2 s corrections to Wγγproduction at the LHC,JHEP12(2025) 221 [2409.08146]

  40. [40]

    Badger, H.B

    S. Badger, H.B. Hartanto, R. Poncelet, Z. Wu, Y. Zhang and S. Zoia,Full-colour double-virtual amplitudes for associated production of a Higgs boson with a bottom-quark pair at the LHC,JHEP03(2025) 066 [2412.06519]

  41. [41]

    A novel approach to integration by parts reduction

    A. von Manteuffel and R.M. Schabinger,A novel approach to integration by parts reduction, Phys. Lett. B744(2015) 101 [1406.4513]

  42. [42]

    Scattering amplitudes over finite fields and multivariate functional reconstruction

    T. Peraro,Scattering amplitudes over finite fields and multivariate functional reconstruction,JHEP12(2016) 030 [1608.01902]

  43. [43]

    Abreu, J

    S. Abreu, J. Dormans, F. Febres Cordero, H. Ita, M. Kraus, B. Page et al.,Caravel: A C++ framework for the computation of multi-loop amplitudes with numerical unitarity, Comput. Phys. Commun.267(2021) 108069 [2009.11957]

  44. [44]

    Ita,Two-loop Integrand Decomposition into Master Integrals and Surface Terms,Phys

    H. Ita,Two-loop Integrand Decomposition into Master Integrals and Surface Terms,Phys. Rev. D94(2016) 116015 [1510.05626]

  45. [45]

    Abreu, F

    S. Abreu, F. Febres Cordero, H. Ita, M. Jaquier, B. Page and M. Zeng,Two-Loop Four-Gluon Amplitudes from Numerical Unitarity,Phys. Rev. Lett.119(2017) 142001 [1703.05273]. – 44 –

  46. [46]

    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 [1703.05255]

  47. [47]

    Abreu, F

    S. Abreu, F. Febres Cordero, H. Ita, B. Page and M. Zeng,Planar Two-Loop Five-Gluon Amplitudes from Numerical Unitarity,Phys. Rev. D97(2018) 116014 [1712.03946]

  48. [48]

    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 [1809.09067]

  49. [49]

    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 [1904.00945]

  50. [50]

    One-Loop n-Point Gauge Theory Amplitudes, Unitarity and Collinear Limits

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

  51. [51]

    Fusing Gauge Theory Tree Amplitudes Into Loop Amplitudes

    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 [hep-ph/9409265]

  52. [52]

    Generalized Unitarity and One-Loop Amplitudes in N=4 Super-Yang-Mills

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

  53. [53]

    Bern, J.J.M

    Z. Bern, J.J.M. Carrasco, H. Johansson and D.A. Kosower,Maximally supersymmetric planar Yang-Mills amplitudes at five loops,Phys. Rev. D76(2007) 125020 [0705.1864]

  54. [54]

    Buchbinder and F

    E.I. Buchbinder and F. Cachazo,Two-loop amplitudes of gluons and octa-cuts in N=4 super Yang-Mills,JHEP11(2005) 036 [hep-th/0506126]

  55. [55]

    Berends and W.T

    F.A. Berends and W.T. Giele,Recursive Calculations for Processes with n Gluons,Nucl. Phys. B306(1988) 759

  56. [56]

    Gluza, K

    J. Gluza, K. Kajda and D.A. Kosower,Towards a Basis for Planar Two-Loop Integrals, Phys. Rev. D83(2011) 045012 [1009.0472]

  57. [57]

    Abreu, G

    S. Abreu, G. De Laurentis, H. Ita, M. Klinkert, B. Page and V. Sotnikov,Two-loop QCD corrections for three-photon production at hadron colliders,SciPost Phys.15(2023) 157 [2305.17056]

  58. [58]

    Klinkert,Two-loop five-point amplitudes for bosons and partons in QCD, Ph.D

    M. Klinkert,Two-loop five-point amplitudes for bosons and partons in QCD, Ph.D. thesis, Freiburg U., 2023. 10.6094/UNIFR/234190

  59. [59]

    De Laurentis, H

    G. De Laurentis, H. Ita, M. Klinkert and V. Sotnikov,Double-virtual NNLO QCD corrections for five-parton scattering. I. The gluon channel,Phys. Rev. D109(2024) 094023 [2311.10086]

  60. [60]

    De Laurentis, H

    G. De Laurentis, H. Ita and V. Sotnikov,Double-virtual NNLO QCD corrections for five-parton scattering. II. The quark channels,Phys. Rev. D109(2024) 094024 [2311.18752]

  61. [61]

    De Laurentis, H

    G. De Laurentis, H. Ita, B. Page and V. Sotnikov,Compact two-loop QCD corrections for Vjj production in proton collisions,JHEP06(2025) 093 [2503.10595]

  62. [62]

    Chicherin, V

    D. Chicherin, V. Sotnikov and S. Zoia,Pentagon functions for one-mass planar scattering amplitudes,JHEP01(2022) 096 [2110.10111]

  63. [63]

    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) 082002 [1812.04586]. – 45 –

  64. [64]

    Laurentis and D

    G. Laurentis and D. Maître,Extracting analytical one-loop amplitudes from numerical evaluations,JHEP07(2019) 123 [1904.04067]

  65. [65]

    De Laurentis and B

    G. De Laurentis and B. Page,Ansätze for scattering amplitudes from p-adic numbers and algebraic geometry,JHEP12(2022) 140 [2203.04269]

  66. [66]

    Abreu, F

    S. Abreu, F. Febres Cordero, H. Ita, B. Page and V. Sotnikov,Leading-color two-loop QCD corrections for three-jet production at hadron colliders,JHEP07(2021) 095 [2102.13609]

  67. [67]

    X. Chen, X. Guan and B. Mistlberger,Three-Loop QCD corrections to the production of a Higgs boson and a Jet,2504.06490

  68. [68]

    Djouadi, M

    A. Djouadi, M. Spira and P.M. Zerwas,Production of Higgs bosons in proton colliders: QCD corrections,Phys. Lett. B264(1991) 440

  69. [69]

    Dawson,Radiative corrections to Higgs boson production,Nucl

    S. Dawson,Radiative corrections to Higgs boson production,Nucl. Phys. B359(1991) 283

  70. [70]

    Kniehl and M

    B.A. Kniehl and M. Spira,Low-energy theorems in Higgs physics,Z. Phys. C69(1995) 77 [hep-ph/9505225]

  71. [71]

    Decoupling Relations to O(alpha_s^3) and their Connection to Low-Energy Theorems

    K.G. Chetyrkin, B.A. Kniehl and M. Steinhauser,Decoupling relations to O (alpha-s**3) and their connection to low-energy theorems,Nucl. Phys. B510(1998) 61 [hep-ph/9708255]

  72. [72]

    Chetyrkin, B.A

    K.G. Chetyrkin, B.A. Kniehl and M. Steinhauser,Hadronic Higgs decay to order alpha-s**4,Phys. Rev. Lett.79(1997) 353 [hep-ph/9705240]

  73. [73]

    Kramer, E

    M. Kramer, E. Laenen and M. Spira,Soft gluon radiation in Higgs boson production at the LHC,Nucl. Phys. B511(1998) 523 [hep-ph/9611272]

  74. [74]

    Gerlach, F

    M. Gerlach, F. Herren and M. Steinhauser,Wilson coefficients for Higgs boson production and decoupling relations toO α4 s ,JHEP11(2018) 141 [1809.06787]

  75. [75]

    K.G. Chetyrkin,A simple generalization of the low-energy theorem for the effective Higgs-gluon-gluon coupling for the case of simultaneous decoupling of several heavy quarks, JHEP02(2026) 192 [2511.20622]

  76. [76]

    Ellis, I

    R.K. Ellis, I. Hinchliffe, M. Soldate and J.J. van der Bij,Higgs Decay toτ+τ −: A Possible Signature of Intermediate Mass Higgs Bosons at SSC,Nucl. Phys. B297(1988) 221

  77. [77]

    Baur and E.W.N

    U. Baur and E.W.N. Glover,Higgs Boson Production at Large Transverse Momentum in Hadronic Collisions,Nucl. Phys. B339(1990) 38

  78. [78]

    Maitre and P

    D. Maitre and P. Mastrolia,S@M, a Mathematica Implementation of the Spinor-Helicity Formalism,Comput. Phys. Commun.179(2008) 501 [0710.5559]

  79. [79]

    Harlander and W.B

    R.V. Harlander and W.B. Kilgore,Soft and virtual corrections to proton proton —>H + x at NNLO,Phys. Rev. D64(2001) 013015 [hep-ph/0102241]

  80. [80]

    Catani,The Singular behavior of QCD amplitudes at two loop order,Phys

    S. Catani,The Singular behavior of QCD amplitudes at two loop order,Phys. Lett. B427 (1998) 161 [hep-ph/9802439]

Showing first 80 references.