NLO EW and QCD corrections to polarized ZZ production in the four-charged-lepton channel at the LHC
arXiv:2107.06579 · doi:10.1007/JHEP10(2021)097
Abstract
Measuring the polarization of electroweak bosons at the LHC allows for important tests of the electroweak-symmetry-breaking mechanism that is realized in nature. Therefore, precise Standard Model predictions are needed for the production of polarized bosons in the presence of realistic kinematic selections. We formulate a method for the calculation of polarized cross-sections at NLO that relies on the pole approximation and the separation of polarized matrix elements at the amplitude level. In this framework, we compute NLO-accurate cross-sections for the production of two polarized Z bosons at the LHC, including for the first time NLO EW corrections and combining them with NLO QCD corrections and contributions from the gluon-induced process.
arXiv comment41 pages, 17 figures, 4 tables, minor corrections w.r.t. v1, matches published version in JHEP
References in corpus (70)
- The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations
- The anti-k_t jet clustering algorithm
- LHAPDF6: parton density access in the LHC precision era
- A General Algorithm for Calculating Jet Cross Sections in NLO QCD
- Parton distributions from high-precision collider data
- Collier: a fortran-based Complex One-Loop LIbrary in Extended Regularizations
- Automatic spin-entangled decays of heavy resonances in Monte Carlo simulations
- The Dipole Formalism for Next-to-Leading Order QCD Calculations with Massive Partons
- Electroweak corrections to charged-current e+e- --> 4 fermion processes - technical details and further results
- ZZ production at hadron colliders in NNLO QCD
- Spin determination of single-produced resonances at hadron colliders
- W+W-, WZ and ZZ production in the POWHEG BOX
- On the spin and parity of a single-produced resonance at the LHC
- A General Approach To Photon Radiation Off Fermions
- RECOLA: REcursive Computation of One-Loop Amplitudes
- Electroweak radiative corrections to e+e- --> WW --> 4fermions in double-pole approximation -- the RACOONWW approach
- Recola2: REcursive Computation of One-Loop Amplitudes 2
- The complex-mass scheme for perturbative calculations with unstable particles
- Illuminating the photon content of the proton within a global PDF analysis
- Identifying the Higgs Spin and Parity in Decays to Z Pairs
- Electroweak Radiative Corrections for Collider Physics
- W+W-, WZ and ZZ production in the POWHEG BOX V2
- Recursive generation of one-loop amplitudes in the Standard Model
- Next-to-leading order calculation of four-jet observables in electron-positron annihilation
- production at the LHC: fiducial cross sections and distributions in NNLO QCD
- QCD corrections to ZZ production in gluon fusion at the LHC
- Vector Boson Pair Production in Hadronic Collisions at Order : Lepton Correlations and Anomalous Couplings
- ZZ production at the LHC: fiducial cross sections and distributions in NNLO QCD
- Prospective Analysis Spin- and CP-sensitive Variables in H -> ZZ -> l_1 l_1 l_2 l_2 with Atlas
- Helicity Amplitudes for Production of or Pairs at Hadron Colliders
- Vector-boson pair production at the LHC to accuracy
- Jet angular correlation in vector-boson fusion processes at hadron colliders
- Narrow-width approximation accuracy
- CP--odd Correlation in the Decay of Neutral Higgs Boson into , , or
- Logarithmic electroweak corrections to gauge-boson pair production at the LHC
- Non-factorizable photonic corrections to ee->WW->4fermions
- Probing CP Violation Via Higgs Decays to Four Leptons
- Left-Handed W Bosons at the LHC
- Electroweak corrections to at the LHC -- a Higgs background study
- PHANTOM: a Monte Carlo event generator for six parton final states at high energy colliders
- NNLO QCD+NLO EW with MATRIX+OpenLoops: precise predictions for vector-boson pair production
- Electroweak gauge boson polarisation at the LHC
- Next-to-leading-order electroweak corrections to the production of four charged leptons at the LHC
- QCD corrections to vector boson pair production in gluon fusion including interference effects with off-shell Higgs at the LHC
- NLO QCD+EW predictions for diboson signatures at the LHC
- production at the LHC: NLO QCD corrections to the loop-induced gluon fusion channel
- Automated Predictions from Polarized Matrix Elements
- production at the LHC: NNLO predictions for and signatures
- ZZ production in gluon fusion at NLO matched to parton-shower
- NNLO predictions for Z-boson pair production at the LHC
- NLO QCD predictions for doubly-polarized WZ production at the LHC
- boson polarization in vector boson scattering at the LHC
- Anomalous triple-gauge-boson interactions in vector-boson pair production with RECOLA2
- Polarized vector boson scattering in the fully leptonic WZ and ZZ channels at the LHC
- Polarized electroweak bosons in production at the LHC including NLO QCD effects
- NLO QCD+NLO EW corrections to diboson production matched to parton shower
- Angular and energy correlations in Higgs decay
- Different polarization definitions in same-sign scattering at the LHC
- NNLO QCD study of polarised production at the LHC
- Combination of the W boson polarization measurements in top quark decays using ATLAS and CMS data at 8 TeV
- Energy Spectra and Energy Correlations in the Decay
- Fiducial polarization observables in hadronic WZ production: A next-to-leading order QCD+EW study
- Vector boson polarizations in the decay of the Standard Model Higgs
- Non-factorizable photonic corrections to resonant production and decay of many unstable particles
- Next-to-next-to-leading order event generation for boson pair production matched to parton shower
- Full NLO QCD corrections to off-shell ttbb production
- Polarization observables in WZ production at the 13 TeV LHC: Inclusive case
- Four-lepton production in gluon fusion at NLO matched to parton showers
- What Does the CMS Measurement of W-polarization Tell Us about the Underlying Theory of the Coupling of W-Bosons to Matter?
- Lepton-mass effects in the decays and