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Xsection 4.1
Xsection 4.1








xsection 4.1
  1. #Xsection 4.1 pdf#
  2. #Xsection 4.1 generator#

The HITRAN2020paper describing the new edition is available in Open Access

xsection 4.1

The top mass approximation uncertainty reported in the last row should not be considered in analyses since it is expected to be covered by the larger mtop scheme uncertainty.The data on this website corresponds to the HITRAN2020 edition of the database. The recommended uncertainties to be considered are PDF, alphaS (combined " PDF+αS unc."), scale and mtop scheme (combined " Scale+mtop unc."). The uncertainties related to missing NNLO finite top-quark mass effects within the FT approximation are also presented (mtop approx.

#Xsection 4.1 pdf#

PDF uncertainties are estimated within the Born-improved approximation and are based on the PDF4LHC15nnlomc set. Uncertainties arising from the choice of renormalization scheme and scale of the top-quark mass (mtop scheme+scale unc.) and their combination with μR and μF variations (comb. Scale uncertainties are obtained by probing six relative variations of μR and μF on top of the central one, i.e. 11 (2022)Ĭurrent recommendations for HH cross-sectionsġ) Inclusive ggF cross sections for Higgs boson pair production are reported below for different centre-of-mass energies in NNLO FTapprox, for m H = 125 GeV with the central scale μ0 = μR = μF = M HH/2 (see ). Resonant: benchmarks for spin-0 HH, SH and SS to be probed with 100-300/fb, including interference with non-resonant HHĪrXiV:2112.12515 J. VBF: cross-sections for ggF HH+2j at hard matrix-element VBF: fiducial cross-sections vs coupling modifiers GgF/VBF: updated cross sections for 13.6TeV, various mH values and new PDF sets GgF: combination of H and HH (in connection with WG2 activities) GgF: NLO EFT frameworks and new shape benchmarks, HEFT vs SMEFT GgF: top-quark mass renormalization scheme uncertainty

#Xsection 4.1 generator#

  • If the ggHH_SMEFT generator is used (User-Processes-V2/ggHH_SMEFT), ref.
  • If predictions within a non-linear EFT are considered, as well as κ λ variations, ref.
  • If the POWHEG generator ggHH is used (User-Processes-V2/ggHH) for SM predictions, ref.
  • It is important to refer also to the implementation of the process in Powheg and not only to the generic Powheg-box paper, in particular: Scyboz,, arXiv:2204.13045.Īssociated production with vector bosons at NNLO. Virtual corrections for NNLO in large-mt limit. NNLL in large-mt limit : please cite if YR4 predictions are used.Ĭombined (mtop + scale) uncertainties. References for production via gluon fusion
  • Deciphering the Nature of the Higgs Sector: CERN-2017-002, arXiv:1610.07922.
  • May 30 - J(workshop in Dubrovnik, Croatia)ĬERN Yellow Reports: Handbook of LHC Higgs Cross Sections:.
  • Decem(part of the annual LHC Higgs WG meeting).
  • September 29-30, 2021 (preparation for HH 2022 workshop next year in Croatia.
  • Novem(part of the annual LHC Higgs WG meeting).
  • Octo(part of the annual LHC Higgs XSWG meeting).
  • September 4-7, 2018 (workshop at Fermilab, USA).
  • Ramona Gröber (06/2018) / Javier Mazzitelli (06/2018) / Maggie Mühlleitner

    xsection 4.1

  • OLD recommendations for gluon fusion (from YR4).
  • Latest recommendations for gluon fusion.
  • xsection 4.1

  • Current recommendations for HH cross-sections.
  • References for production via gluon fusion.









  • Xsection 4.1