Electroweak corrections to Higgs-strahlung off W/Z bosons at the Tevatron and the LHC with Hawk
By Ansgar Denner, Stefan Dittmaier, Stefan Kallweit, A. Mück. 2011
304 citations recorded by the source corpus.
A bstractThe associate production of Higgs bosons with W or Z bosons, known as Higgs-strahlung, is an important search channel for Higgs bosons at the hadron colliders Tevatron and LHC for low Higgs-boson masses. We refine a previous calculation of next-to-leading-order electroweak corrections (and recalculate the QCD corrections) upon including the leptonic decay of the W/Z bosons, thereby keeping the fully differential information of the 2-lepton + Higgs final state. The gauge invariance of the W/Z-resonance treatment is ensured by the use of the complex-mass scheme. The electroweak corrections, which are at the level of − (5−10)% for total cross sections, further increase in size with increasing transverse momenta pT in differential cross sections. For instance, for pT,H$ {\underset{\raise0.3em\hbox{$\smash{\scriptscriptstyle\thicksim}$}}{ > }} $ 200 GeV, which is the interesting range at the LHC, the electroweak corrections to WH production reach about −14% for MH = 120 GeV. The described corrections are implemented in the Hawk Monte Carlo program, which was initially designed for the vector-boson-fusion channel, and are discussed for various distributions in the production channels $ {\text{pp}}/{\text{p}}\overline {\text{p}} \to {\text{H}} + l{{v}_{l}}{{l}^{ - }}{{l}^{ + }}/ + X $.
Subfields: Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/c01cd3c39a09e98a2a195d225ee745c08749689f
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In Nuclear and High Energy Physics
- Atlas Collaboration
- Cms Collaboration
- Gudrun Heinrich
- M. Schönherr
- Fabio Maltoni
- Stefan Dittmaier
- Ansgar Denner
- F. Krauss
Citations in the corpus
- Physics at a 100 TeV pp collider: Higgs and EW symmetry breaking studies (2016, methodology): “Furthermore, programs have been developed for the computation of fully differential distributions including NNLO QCD corrections [100–103], the EW corrections [104, 105] and event generators matching and merging NLO QCD corrections for VH+jets production to parton showers [106–108].”
- Measurements of the Higgs boson production and decay rates and coupling strengths using pp collision data at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\o (2015, unknown): “The cross sections of the WH and ZH (qq̄ → ZH ) are calculated including QCD corrections up to NNLO [53,54] and EW corrections up to NLO [55,56] whereas the cross section of the gg → ZH process is calculated up to NLO in QCD corrections [57,58].”
- The measurement of the Higgs self-coupling at the LHC: theoretical status (2012, unknown): “energies [67–76] (see also ref.”
- Handbook of LHC Higgs Cross Sections: 3. Higgs Properties (2013, unknown): “1 HAWK HAWK is a parton-level event generator for Higgs production in vector-boson fusion [104–106], pp → Hjj, and Higgs-strahlung [107], pp → WH → νl l H andpp → ZH → llH/νlνlH.”
- Search for exclusive Higgs and Z boson decays to ϕγ and ργ with the ATLAS detector (2017, methodology): “The W H and Z H production rates are normalised to cross sections calculated at NNLO in QCDwith NLO electroweak corrections [50, 51] including the NLOQCD corrections [52] for gg → Z H .”
- Associated production of a Higgs boson at NNLO (2016, background): “[12, 13] while resummation effects have been studied in refs.”
- The photon content of the proton (2017, background): “Some notable examples are the production of the Higgs boson through W/Z fusion [1], or in association with an outgoing weak boson [2].”
- Gluon-induced Higgs-strahlung at next-to-leading order QCD (2012, methodology): “[13] for differential distributions as part of the HAWK Monte Carlo program, which fully includes all decays and off-shell effects of the weak boson V = W,Z.”
- Higgs Physics at the HL-LHC and HE-LHC (2019, methodology): “The results have been obtained using HAWK, combining NNLO QCD and NLO EW corrections [64, 63, 65, 66, 67, 68, 69], by means of a multiplicative scheme, as described in the YR4 studies (eq.”