First N³LO QCD prediction for boosted WH production yields +2% corrections with sub-percent residual scale dependence.
NNLO QCD corrections to associated $WH$ production and $H \to b \bar b$ decay
6 Pith papers cite this work. Polarity classification is still indexing.
abstract
We present a computation of the next-to-next-to-leading order (NNLO) QCD corrections to the production of a Higgs boson in association with a W boson at the LHC and the subsequent decay of the Higgs boson into a b-bbar pair, treating the b-quarks as massless. We consider various kinematic distributions and find significant corrections to observables that resolve the Higgs decay products. We also find that a cut on the transverse momentum of the W boson, important for experimental analyses, may have a significant impact on kinematic distributions and radiative corrections. We show that some of these effects can be adequately described by simulating QCD radiation in Higgs boson decays to b-quarks using parton showers. We also describe contributions to Higgs decay to a b-bbar pair that first appear at NNLO and that were not considered in previous fully-differential computations. The calculation of NNLO QCD corrections to production and decay sub-processes is carried out within the nested soft-collinear subtraction scheme presented by some of us earlier this year. We demonstrate that this subtraction scheme performs very well, allowing a computation of the coefficient of the second order QCD corrections at the level of a few per mill.
citation-role summary
citation-polarity summary
fields
hep-ph 6roles
background 1polarities
background 1representative citing papers
First NNLO QCD predictions for WH plus jet production at 13 TeV, including top-quark loop effects, yield inclusive cross sections stable at the 1% level.
The thesis computes three-loop and two-loop QCD corrections to Higgs processes with full quark mass dependence, including a new analytic series-expansion treatment of elliptic two-loop master integrals for Higgs-plus-jet production.
A new NNLL'-resummed 2-jettiness calculation for H→bb and H→gg decays, matched to NNLO and a parton shower in the GENEVA framework, yielding fully exclusive NNLO event generators.
GENEVA now generates Higgsstrahlung events at NNLO accuracy matched with NNLL' beam-thrust resummation and parton showers, validated against Matrix for the 13 TeV LHC.
The report reviews progress since 2021 in fixed-order computations for LHC applications and identifies processes requiring missing higher-order corrections to match anticipated experimental precision.
citing papers explorer
-
Boosted Higgs-strahlung off a $W$ boson at next-to-next-to-next-to-leading order in QCD
First N³LO QCD prediction for boosted WH production yields +2% corrections with sub-percent residual scale dependence.
-
Precise predictions for $\mathrm{WH}$+jet production at the LHC
First NNLO QCD predictions for WH plus jet production at 13 TeV, including top-quark loop effects, yield inclusive cross sections stable at the 1% level.
-
Higher-Order Corrections to Higgs Boson Amplitudes with Full Quark Mass Dependence in Quantum Chromodynamics
The thesis computes three-loop and two-loop QCD corrections to Higgs processes with full quark mass dependence, including a new analytic series-expansion treatment of elliptic two-loop master integrals for Higgs-plus-jet production.
-
Resummed predictions for hadronic Higgs boson decays
A new NNLL'-resummed 2-jettiness calculation for H→bb and H→gg decays, matched to NNLO and a parton shower in the GENEVA framework, yielding fully exclusive NNLO event generators.
-
Higgsstrahlung at NNLL$'+$NNLO Matched to Parton Showers in GENEVA
GENEVA now generates Higgsstrahlung events at NNLO accuracy matched with NNLL' beam-thrust resummation and parton showers, validated against Matrix for the 13 TeV LHC.
-
Les Houches 2023 -- Physics at TeV Colliders: Report on the Standard Model Precision Wishlist
The report reviews progress since 2021 in fixed-order computations for LHC applications and identifies processes requiring missing higher-order corrections to match anticipated experimental precision.