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arxiv: 2606.31286 · v1 · pith:A2LXOGGQnew · submitted 2026-06-30 · ✦ hep-ph

Boosted Higgs-strahlung off a W boson at next-to-next-to-next-to-leading order in QCD

Aude Gehrmann-De Ridder , Alexander Huss , Matteo Marcoli , Pier Francesco Monni , Emanuele Re , Luca Rottoli , Federico Silvetti , Paolo Torrielli This is my paper

Pith reviewed 2026-07-01 05:08 UTC · model grok-4.3

classification ✦ hep-ph
keywords Higgs productionN3LO QCDboosted regimeWH associated productionperturbative correctionshadron collidersdifferential cross section
8
0 comments X

The pith

The first fully differential N³LO QCD calculation for boosted Higgs plus W production finds corrections of about +2% that sit at or beyond the NNLO scale-variation band.

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

The paper delivers the first fully differential computation of Higgs-strahlung off a W boson at next-to-next-to-next-to-leading order in QCD. In the boosted regime the N³LO corrections reach approximately +2% and typically lie at the edge of or outside the uncertainty band obtained from scale variation at the preceding order. At the same time the residual dependence on perturbative scales falls below the percent level. This combination tightens the theoretical prediction for a channel that dominates Higgs production at large transverse momentum and supplies direct sensitivity to Higgs couplings and possible new physics.

Core claim

We present the first fully differential calculation of boosted Higgs-strahlung off a W boson at N³LO in perturbative QCD. The N³LO corrections amount to approximately +2% in the boosted regime and generally lie at the edge of or outside the standard scale variation band of the previous perturbative order, while the residual dependence of the N³LO prediction on perturbative scales is reduced to below the percent level.

What carries the argument

The fully differential N³LO QCD computation of the pp → WH cross section, incorporating all virtual and real-emission contributions through third order in the strong coupling.

Load-bearing premise

That the conventional scale-variation procedure performed at NNLO supplies a reliable estimate of the size of the missing higher-order corrections.

What would settle it

A high-precision measurement of the boosted WH cross section whose central value lies well inside the NNLO scale band but outside the N³LO prediction band.

Figures

Figures reproduced from arXiv: 2606.31286 by Alexander Huss, Aude Gehrmann-De Ridder, Emanuele Re, Federico Silvetti, Luca Rottoli, Matteo Marcoli, Paolo Torrielli, Pier Francesco Monni.

Figure 1
Figure 1. Figure 1: FIG. 1: (a) Born-level Feynman diagram for the [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2: N [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3: Fiducial [PITH_FULL_IMAGE:figures/full_fig_p005_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: , we show the N3LO correction to the inclusive cross section as a function of q cut T , decomposed into initial￾state flavor channels and compared with the numerical results of n3loxs. We find excellent agreement across the full range 3 GeV ≤ q cut T ≤ 10 GeV, with residual variations well within the Monte Carlo integration uncertainty of the N3LO correction. The latter reaches at most ±30% in the qq¯ chan… view at source ↗
read the original abstract

The production of a boosted Higgs boson in association with a charged weak ($W$) boson is a key process to scrutinize the electroweak symmetry breaking mechanism at hadron colliders. This reaction constitutes the dominant Higgs production channel at large transverse momentum, providing unique sensitivity to Higgs-boson interactions with other Standard Model particles as well as to physics beyond the Standard Model. In this Letter, we present the first fully differential calculation of this important scattering process at next-to-next-to-next-to-leading order (N$^3$LO) in perturbative Quantum Chromodynamics (QCD). We find that the N$^3$LO corrections, amounting to approximately $+2\%$ in the boosted regime, generally lie at the edge of or outside the standard scale variation band of the previous perturbative order. The residual dependence of the N$^3$LO prediction on perturbative scales is reduced to below the percent level, marking a milestone for the Higgs precision program.

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 manuscript presents the first fully differential N³LO QCD calculation of Higgs-strahlung off a W boson (WH production) in the boosted Higgs regime at hadron colliders. The central numerical result is that N³LO corrections amount to approximately +2% and generally lie at the edge of or outside the NNLO scale-variation band, while reducing residual perturbative scale dependence to below the percent level.

Significance. If the result holds, this constitutes a milestone for precision Higgs phenomenology, as boosted WH is the dominant production mode at high pT and provides direct sensitivity to Higgs couplings and potential BSM effects. Achieving sub-percent residual scale uncertainty supplies more robust theoretical inputs for LHC analyses than previous orders.

major comments (1)
  1. [Abstract] Abstract: The statement that the N³LO corrections 'generally lie at the edge of or outside the standard scale variation band of the previous perturbative order' rests on the assumption that the conventional 7-point scale variation performed at NNLO furnishes a faithful envelope for the size of the uncalculated N³LO terms. The manuscript provides no independent cross-check of this assumption (e.g., via an alternative uncertainty prescription, comparison against a known N³LO process, or explicit demonstration in a solvable limit). This directly affects the strength of the claim that the N³LO shift lies outside the previous uncertainty estimate.
minor comments (1)
  1. [Abstract] The abstract would benefit from a brief statement of the collider energy and the precise kinematic definition of the 'boosted regime' used for the quoted +2% correction.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the careful reading of our manuscript and the positive overall assessment. We address the major comment below.

read point-by-point responses

  1. Referee: [Abstract] Abstract: The statement that the N³LO corrections 'generally lie at the edge of or outside the standard scale variation band of the previous perturbative order' rests on the assumption that the conventional 7-point scale variation performed at NNLO furnishes a faithful envelope for the size of the uncalculated N³LO terms. The manuscript provides no independent cross-check of this assumption (e.g., via an alternative uncertainty prescription, comparison against a known N³LO process, or explicit demonstration in a solvable limit). This directly affects the strength of the claim that the N³LO shift lies outside the previous uncertainty estimate.

    Authors: We agree that conventional 7-point scale variation provides an estimate of higher-order effects rather than a rigorous bound, and that the manuscript does not include an independent cross-check such as an alternative prescription or comparison to a different N³LO process. Our statement is an empirical observation based on the explicit computation: the N³LO correction size is compared directly to the NNLO 7-point band obtained with the same scale choices. This follows the standard practice used in all prior N³LO QCD calculations. In the revised manuscript we have added a clarifying sentence after the abstract claim noting that the observation relies on the conventional scale-variation prescription and does not constitute a general proof. We have also softened the wording slightly to 'lie at or beyond the edge of the NNLO scale-variation band obtained with the standard 7-point prescription.' We believe this addresses the concern without altering the numerical results or the main conclusions. revision: partial

Circularity Check

0 steps flagged

No circularity: direct N³LO perturbative computation

full rationale

The paper reports an explicit higher-order QCD calculation of differential distributions for WH production at N³LO. All results follow from standard matrix-element evaluation, infrared subtraction, and phase-space integration; no quantity is obtained by fitting a parameter to a subset of the same data and then relabeling it a prediction, nor does any central claim reduce to a self-citation chain or imported ansatz. Scale variation is used only as a conventional uncertainty estimate after the calculation is complete and does not enter the derivation itself.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The calculation rests on standard perturbative QCD assumptions; no new entities or data-fitted parameters are introduced beyond conventional scale choices.

free parameters (1)
  • renormalization and factorization scales
    Standard choices in pQCD; varied to estimate uncertainty but not fitted to data.
axioms (1)
  • domain assumption Perturbative QCD expansion remains valid and convergent at N³LO for this process
    Invoked throughout the abstract to justify the calculation and uncertainty reduction.

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Works this paper leans on

89 extracted references · 86 canonical work pages · 38 internal anchors

  1. [1]

    Aadet al.(ATLAS), Eur

    G. Aadet al.(ATLAS), Eur. Phys. J. C81, 178 (2021), arXiv:2007.02873 [hep-ex]

    work page arXiv 2021

  2. [2]

    Aadet al.(ATLAS), Phys

    G. Aadet al.(ATLAS), Phys. Rev. D105, 092003 (2022), arXiv:2111.08340 [hep-ex]

    work page arXiv 2022

  3. [3]

    Aadet al.(ATLAS), Phys

    G. Aadet al.(ATLAS), Phys. Rev. Lett.132, 131802 (2024), arXiv:2312.07605 [hep-ex]

    work page arXiv 2024

  4. [4]

    A. M. Sirunyanet al.(CMS), JHEP12, 085, arXiv:2006.13251 [hep-ex]

    work page arXiv 2006

  5. [5]

    A. M. Sirunyanet al.(CMS), Phys. Rev. D104, 052004 (2021), arXiv:2104.12152 [hep-ex]

    work page arXiv 2021

  6. [6]

    Hayrapetyanet al.(CMS), JHEP12, 035, arXiv:2407.08012 [hep-ex]

    A. Hayrapetyanet al.(CMS), JHEP12, 035, arXiv:2407.08012 [hep-ex]

    work page arXiv

  7. [7]

    Baglio, S

    J. Baglio, S. Dawson, S. Homiller, S. D. Lane, and I. M. Lewis, Phys. Rev. D101, 115004 (2020), arXiv:2003.07862 [hep-ph]

    work page arXiv 2020

  8. [8]

    Constraints on the trilinear Higgs coupling from vector boson fusion and associated Higgs production at the LHC

    W. Bizon, M. Gorbahn, U. Haisch, and G. Zanderighi, JHEP07, 083, arXiv:1610.05771 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv

  9. [9]

    Bizo´ n, F

    W. Bizo´ n, F. Caola, K. Melnikov, and R. R¨ ontsch, Phys. Rev. D105, 014023 (2022), arXiv:2106.06328 [hep-ph]

    work page arXiv 2022

  10. [10]

    Gauld, U

    R. Gauld, U. Haisch, and L. Schnell, JHEP01, 192, arXiv:2311.06107 [hep-ph]

    work page arXiv

  11. [11]

    Bonetti, R

    M. Bonetti, R. V. Harlander, D. Korneev, M.-M. Long, K. Melnikov, R. R¨ ontsch, and D. M. Tagliabue, Phys. Rev. D112, 034033 (2025), arXiv:2502.12846 [hep-ph]

    work page arXiv 2025

  12. [12]

    Beckeret al., SciPost Phys

    K. Beckeret al., SciPost Phys. Core7, 001 (2024), arXiv:2005.07762 [hep-ph]

    work page arXiv 2024

  13. [13]

    Baglio, C

    J. Baglio, C. Duhr, B. Mistlberger, and R. Szafron, JHEP 12, 066, arXiv:2209.06138 [hep-ph]

    work page arXiv

  14. [14]

    M. L. Ciccolini, S. Dittmaier, and M. Kramer, Phys. Rev. D68, 073003 (2003), arXiv:hep-ph/0306234

    work page internal anchor Pith review Pith/arXiv arXiv 2003

  15. [15]

    Electroweak corrections to Higgs-strahlung off W/Z bosons at the Tevatron and the LHC with HAWK

    A. Denner, S. Dittmaier, S. Kallweit, and A. Muck, JHEP 03, 075, arXiv:1112.5142 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv

  16. [16]

    HAWK 2.0: A Monte Carlo program for Higgs production in vector-boson fusion and Higgs strahlung at hadron colliders

    A. Denner, S. Dittmaier, S. Kallweit, and A. M¨ uck, Com- put. Phys. Commun.195, 161 (2015), arXiv:1412.5390 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2015

  17. [17]

    NLO QCD+EW predictions for HV and HV+jet production including parton-shower effects

    F. Granata, J. M. Lindert, C. Oleari, and S. Pozzorini, 6 JHEP09, 012, arXiv:1706.03522 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv

  18. [18]

    Associated WH production at hadron colliders: a fully exclusive QCD calculation at NNLO

    G. Ferrera, M. Grazzini, and F. Tramontano, Phys. Rev. Lett.107, 152003 (2011), arXiv:1107.1164 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2011

  19. [19]

    Higher-order QCD effects for associated WH production and decay at the LHC

    G. Ferrera, M. Grazzini, and F. Tramontano, JHEP04, 039, arXiv:1312.1669 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv

  20. [20]

    NNLOPS accurate associated HW production

    W. Astill, W. Bizon, E. Re, and G. Zanderighi, JHEP 06, 154, arXiv:1603.01620 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv

  21. [21]

    J. M. Campbell, R. K. Ellis, and C. Williams, JHEP06, 179, arXiv:1601.00658 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv

  22. [22]

    NNLO QCD corrections to associated $WH$ production and $H \to b \bar b$ decay

    F. Caola, G. Luisoni, K. Melnikov, and R. R¨ ontsch, Phys. Rev. D97, 074022 (2018), arXiv:1712.06954 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2018

  23. [23]

    Associated production of a Higgs boson decaying into bottom quarks at the LHC in full NNLO QCD

    G. Ferrera, G. Somogyi, and F. Tramontano, Phys. Lett. B780, 346 (2018), arXiv:1705.10304 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2018

  24. [24]

    Alioli, A

    S. Alioli, A. Broggio, S. Kallweit, M. A. Lim, and L. Rot- toli, Phys. Rev. D100, 096016 (2019), arXiv:1909.02026 [hep-ph]

    work page arXiv 2019

  25. [25]

    Behring, W

    A. Behring, W. Bizo´ n, F. Caola, K. Melnikov, and R. R¨ ontsch, Phys. Rev. D101, 114012 (2020), arXiv:2003.08321 [hep-ph]

    work page arXiv 2020

  26. [26]

    Majer,Associated Higgs Boson Production at NNLO QCD, Ph.D

    I. Majer,Associated Higgs Boson Production at NNLO QCD, Ph.D. thesis, Zurich, ETH, Zurich, ETH (2020)

    2020

  27. [27]

    Zanoli, M

    S. Zanoli, M. Chiesa, E. Re, M. Wiesemann, and G. Zan- derighi, JHEP07, 008, arXiv:2112.04168 [hep-ph]

    work page arXiv

  28. [28]

    Gauld, A

    R. Gauld, A. Gehrmann-De Ridder, E. W. N. Glover, A. Huss, and I. Majer, JHEP10, 002, arXiv:1907.05836 [hep-ph]

    work page arXiv 1907

  29. [29]

    Haisch, D

    U. Haisch, D. J. Scott, M. Wiesemann, G. Zanderighi, and S. Zanoli, JHEP07, 054, arXiv:2204.00663 [hep-ph]

    work page arXiv

  30. [30]

    Higgs boson gluon-fusion production in N3LO QCD

    C. Anastasiou, C. Duhr, F. Dulat, F. Herzog, and B. Mistlberger, Phys. Rev. Lett.114, 212001 (2015), arXiv:1503.06056 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2015

  31. [31]

    High precision determination of the gluon fusion Higgs boson cross-section at the LHC

    C. Anastasiou, C. Duhr, F. Dulat, E. Furlan, T. Gehrmann, F. Herzog, A. Lazopoulos, and B. Mistl- berger, JHEP05, 058, arXiv:1602.00695 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv

  32. [32]

    F. A. Dreyer and A. Karlberg, Phys. Rev. Lett.117, 072001 (2016), arXiv:1606.00840 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2016

  33. [33]

    Higgs Boson Production at Hadron Colliders at N3LO in QCD

    B. Mistlberger, JHEP05, 028, arXiv:1802.00833 [hep- ph]

    work page internal anchor Pith review Pith/arXiv arXiv

  34. [34]

    F. A. Dreyer and A. Karlberg, Phys. Rev. D98, 114016 (2018), arXiv:1811.07906 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2018

  35. [35]

    Higgs boson production at the LHC using the $q_T$ subtraction formalism at N$^3$LO QCD

    L. Cieri, X. Chen, T. Gehrmann, E. W. N. Glover, and A. Huss, JHEP02, 096, arXiv:1807.11501 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv

  36. [36]

    L.-B. Chen, H. T. Li, H.-S. Shao, and J. Wang, Phys. Lett. B803, 135292 (2020), arXiv:1909.06808 [hep-ph]

    work page arXiv 2020

  37. [37]

    L.-B. Chen, H. T. Li, H.-S. Shao, and J. Wang, JHEP 03, 072, arXiv:1912.13001 [hep-ph]

    work page arXiv 1912

  38. [38]

    C. Duhr, F. Dulat, and B. Mistlberger, Phys. Rev. Lett. 125, 051804 (2020), arXiv:1904.09990 [hep-ph]

    work page arXiv 2020

  39. [39]

    C. Duhr, F. Dulat, and B. Mistlberger, JHEP11, 143, arXiv:2007.13313 [hep-ph]

    work page arXiv 2007

  40. [40]

    Duhr and B

    C. Duhr and B. Mistlberger, JHEP03, 116, arXiv:2111.10379 [hep-ph]

    work page arXiv

  41. [41]

    X. Chen, T. Gehrmann, E. W. N. Glover, A. Huss, B. Mistlberger, and A. Pelloni, Phys. Rev. Lett.127, 072002 (2021), arXiv:2102.07607 [hep-ph]

    work page arXiv 2021

  42. [42]

    Billis, B

    G. Billis, B. Dehnadi, M. A. Ebert, J. K. L. Michel, and F. J. Tackmann, Phys. Rev. Lett.127, 072001 (2021), arXiv:2102.08039 [hep-ph]

    work page arXiv 2021

  43. [43]

    Camarda, L

    S. Camarda, L. Cieri, and G. Ferrera, Phys. Rev. D104, L111503 (2021), arXiv:2103.04974 [hep-ph]

    work page arXiv 2021

  44. [44]

    X. Chen, T. Gehrmann, N. Glover, A. Huss, T.-Z. Yang, and H. X. Zhu, Phys. Rev. Lett.128, 052001 (2022), arXiv:2107.09085 [hep-ph]

    work page arXiv 2022

  45. [45]

    X. Chen, T. Gehrmann, E. W. N. Glover, A. Huss, P. F. Monni, E. Re, L. Rottoli, and P. Torrielli, Phys. Rev. Lett.128, 252001 (2022), arXiv:2203.01565 [hep-ph]

    work page arXiv 2022

  46. [46]

    Neumann and J

    T. Neumann and J. Campbell, Phys. Rev. D107, L011506 (2023), arXiv:2207.07056 [hep-ph]

    work page arXiv 2023

  47. [47]

    X. Chen, T. Gehrmann, N. Glover, A. Huss, T.-Z. Yang, and H. X. Zhu, Phys. Lett. B840, 137876 (2023), arXiv:2205.11426 [hep-ph]

    work page arXiv 2023

  48. [48]

    Campbell and T

    J. Campbell and T. Neumann, JHEP11, 127, arXiv:2308.15382 [hep-ph]

    work page arXiv

  49. [49]

    Next-to-next-to-next-to-leading order QCD corrections to photon-pair production

    M. Czakon, F. Eschment, T. Generet, and R. Poncelet, (2026), arXiv:2604.12613 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2026

  50. [50]

    X. Chen, Y. Dai, H. T. Li, S.-Y. Li, H.-S. Shao, and J. Wang, (2026), arXiv:2601.19990 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2026

  51. [51]

    An NNLO subtraction formalism in hadron collisions and its application to Higgs boson production at the LHC

    S. Catani and M. Grazzini, Phys. Rev. Lett.98, 222002 (2007), arXiv:hep-ph/0703012

    work page internal anchor Pith review Pith/arXiv arXiv 2007

  52. [52]

    Gehrmann, E

    T. Gehrmann, E. W. N. Glover, T. Huber, N. Ikizlerli, and C. Studerus, JHEP06, 094, arXiv:1004.3653 [hep- ph]

    work page arXiv

  53. [53]

    Vector boson production at hadron colliders: hard-collinear coefficients at the NNLO

    S. Catani, L. Cieri, D. de Florian, G. Ferrera, and M. Grazzini, Eur. Phys. J. C72, 2195 (2012), arXiv:1209.0158 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2012

  54. [54]

    Gehrmann, T

    T. Gehrmann, T. Luebbert, and L. L. Yang, JHEP06, 155, arXiv:1403.6451 [hep-ph]

    work page arXiv

  55. [55]

    Rapidity renormalized TMD soft and beam functions at two loops

    T. L¨ ubbert, J. Oredsson, and M. Stahlhofen, JHEP03, 168, arXiv:1602.01829 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv

  56. [56]

    M. G. Echevarria, I. Scimemi, and A. Vladimirov, JHEP 09, 004, arXiv:1604.07869 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv

  57. [57]

    Bootstrapping rapidity anomalous dimension for transverse-momentum resummation

    Y. Li and H. X. Zhu, Phys. Rev. Lett.118, 022004 (2017), arXiv:1604.01404 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2017

  58. [58]

    A. A. Vladimirov, Phys. Rev. Lett.118, 062001 (2017), arXiv:1610.05791 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2017

  59. [59]

    Luo, T.-Z

    M.-x. Luo, T.-Z. Yang, H. X. Zhu, and Y. J. Zhu, Phys. Rev. Lett.124, 092001 (2020), arXiv:1912.05778 [hep- ph]

    work page arXiv 2020

  60. [60]

    M. A. Ebert, B. Mistlberger, and G. Vita, JHEP09, 146, arXiv:2006.05329 [hep-ph]

    work page arXiv 2006

  61. [61]

    Luo, T.-Z

    M.-x. Luo, T.-Z. Yang, H. X. Zhu, and Y. J. Zhu, JHEP 06, 115, arXiv:2012.03256 [hep-ph]

    work page arXiv 2012

  62. [62]

    P. F. Monni, E. Re, and P. Torrielli, Phys. Rev. Lett. 116, 242001 (2016), arXiv:1604.02191 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2016

  63. [63]

    Bizon, P

    W. Bizon, P. F. Monni, E. Re, L. Rottoli, and P. Torrielli, JHEP02, 108, arXiv:1705.09127 [hep-ph]

    work page arXiv

  64. [64]

    E. Re, L. Rottoli, and P. Torrielli, JHEP2109, 108, arXiv:2104.07509 [hep-ph]

    work page arXiv

  65. [65]

    NNLOJET: a parton-level event generator for jet cross sections at NNLO QCD accuracy

    A. Husset al.(NNLOJET), SciPost Phys. Codeb.69, 1 (2026), arXiv:2503.22804 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2026

  66. [66]

    Antenna Subtraction at NNLO

    A. Gehrmann-De Ridder, T. Gehrmann, and E. W. N. Glover, JHEP09, 056, arXiv:hep-ph/0505111

    work page internal anchor Pith review Pith/arXiv arXiv

  67. [67]

    Infrared Structure at NNLO Using Antenna Subtraction

    J. Currie, E. W. N. Glover, and S. Wells, JHEP04, 066, arXiv:1301.4693 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv

  68. [68]

    Gauld, A

    R. Gauld, A. Gehrmann-De Ridder, E. W. N. Glover, A. Huss, and I. Majer, Phys. Lett. B817, 136335 (2021), arXiv:2009.14209 [hep-ph]

    work page arXiv 2021

  69. [69]

    Gauld, A

    R. Gauld, A. Gehrmann-De Ridder, E. W. N. Glover, A. Huss, and I. Majer, JHEP03, 008, arXiv:2110.12992 [hep-ph]

    work page arXiv

  70. [70]

    Buccioni, J.-N

    F. Buccioni, J.-N. Lang, J. M. Lindert, P. Maierh¨ ofer, S. Pozzorini, H. Zhang, and M. F. Zoller, Eur. Phys. J. C79, 866 (2019), arXiv:1907.13071 [hep-ph]

    work page arXiv 2019

  71. [71]

    Top-Quark Mediated Effects in Hadronic Higgs-Strahlung

    O. Brein, R. Harlander, M. Wiesemann, and T. Zirke, Eur. Phys. J. C72, 1868 (2012), arXiv:1111.0761 [hep- ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2012

  72. [72]

    R. D. Ballet al.(NNPDF), Eur. Phys. J. C84, 659 (2024), arXiv:2402.18635 [hep-ph]. 7

    work page arXiv 2024

  73. [73]

    LHAPDF6: parton density access in the LHC precision era

    A. Buckley, J. Ferrando, S. Lloyd, K. Nordstr¨ om, B. Page, M. R¨ ufenacht, M. Sch¨ onherr, and G. Watt, Eur. Phys. J. C75, 132 (2015), arXiv:1412.7420 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2015

  74. [74]

    LHCHXSWG, Higgs production cross section for run iii (2025)

    2025

  75. [75]

    J. R. Andersenet al., in9th Les Houches Workshop on Physics at TeV Colliders(2016) arXiv:1605.04692 [hep- ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2016

  76. [76]

    Bergeret al., SciPost Phys

    N. Bergeret al., SciPost Phys. Comm. Rep. 10.21468/Sci- PostPhysCommRep.15 (2019), arXiv:1906.02754 [hep- ph]

    work page doi:10.21468/sci- 2019

  77. [77]

    Measurement of $VH$, $H\to b\bar{b}$ production as a function of the vector-boson transverse momentum in 13 TeV $pp$ collisions with the ATLAS detector

    M. Aaboudet al.(ATLAS), JHEP05, 141, arXiv:1903.04618 [hep-ex]

    work page internal anchor Pith review Pith/arXiv arXiv 1903

  78. [78]

    Gehrmann-De Ridder, A

    A. Gehrmann-De Ridder, A. Huss, M. Marcoli, P. F. Monni, E. Re, L. Rottoli, F. Silvetti, and P. Torrielli, (2026), Supplemental Material to this Letter

    2026

  79. [79]

    Constraints on the polarized gluon density in the proton from charm photoproduction

    S. Frixione and G. Ridolfi, Phys. Lett. B383, 227 (1996), arXiv:hep-ph/9605209

    work page internal anchor Pith review Pith/arXiv arXiv 1996

  80. [80]

    Fully differential NNLO computations with MATRIX

    M. Grazzini, S. Kallweit, and M. Wiesemann, Eur. Phys. J. C78, 537 (2018), arXiv:1711.06631 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2018

Showing first 80 references.