0000000000189909

AUTHOR

Stefan Kallweit

0000-0001-8706-3976

showing 7 related works from this author

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

2014

The Monte Carlo integrator HAWK provides precision predictions for Higgs production at hadron colliders in vector-boson fusion and Higgs strahlung, i.e. in production processes where the Higgs boson is Attached to WeaK bosons. The fully differential predictions include the full QCD and electroweak next-to-leading-order corrections. Results are computed as integrated cross sections and as binned distributions for important hadron-collider observables.

Quantum chromodynamicsPhysicsParticle physicsLarge Hadron ColliderHigh Energy Physics::LatticeElectroweak interactionMonte Carlo methodHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyFOS: Physical sciencesVector bosonHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Hardware and ArchitectureHiggs bosonMonte Carlo integrationHigh Energy Physics::ExperimentBoson
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ZZ production at the LHC: Fiducial cross sections and distributions in NNLO QCD

2015

We consider QCD radiative corrections to the production of four charged leptons in the ZZ signal region at the LHC. We report on the complete calculation of the next-to-next-to-leading order (NNLO) corrections to this process in QCD perturbation theory. Numerical results are presented for $\sqrt{s}=8$ TeV, using typical selection cuts applied by the ATLAS and CMS collaborations. The NNLO corrections increase the NLO fiducial cross section by about $15\%$, and they have a relatively small impact on the shape of the considered kinematical distributions. In the case of the $\Delta\Phi$ distribution of the two Z candidates, the NNLO corrections improve the agreement of the theoretical predictio…

Nuclear and High Energy Physics530 Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciences10192 Physics Institute01 natural scienceslcsh:QC1-999High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::Experiment3106 Nuclear and High Energy Physics010306 general physicslcsh:PhysicsPhysics Letters B
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ZZ production at hadron colliders in NNLO QCD

2014

We report on the first calculation of next-to-next-to-leading order (NNLO) QCD corrections to the inclusive production of ZZ pairs at hadron colliders. Numerical results are presented for pp collisions with centre-of-mass energy ($\sqrt{s}$) ranging from 7 to 14 TeV. The NNLO corrections increase the NLO result by an amount varying from $11\%$ to $17\%$ as $\sqrt{s}$ goes from 7 to 14 TeV. The loop-induced gluon fusion contribution provides about $60\%$ of the total NNLO effect. When going from NLO to NNLO the scale uncertainties do not decrease and remain at the $\pm 3\%$ level.

PhysicsScattering cross-sectionQuantum chromodynamicsParticle physicsNuclear and High Energy PhysicsLarge Hadron Collider010308 nuclear & particles physics530 PhysicsComputationHadronHigh Energy Physics::PhenomenologyNuclear TheoryFOS: Physical sciences10192 Physics Institute7. Clean energy01 natural sciencesNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesRadiative transferHigh Energy Physics::Experiment3106 Nuclear and High Energy Physics010306 general physicsNuclear ExperimentPHYSICS LETTERS B
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W+W−Production at Hadron Colliders in Next to Next to Leading Order QCD

2014

Charged gauge boson pair production at the Large Hadron Collider allows detailed probes of the fundamental structure of electroweak interactions. We present precise theoretical predictions for on-shell W+ W- production that include, for the first time, QCD effects up to next to next to leading order in perturbation theory. As compared to next to leading order, the inclusive W+ W- cross section is enhanced by 9% at 7 TeV and 12% at 14 TeV. The residual perturbative uncertainty is at the 3% level. The severe contamination of the W+ W- cross section due to top-quark resonances is discussed in detail. Comparing different definitions of top-free W+ W- production in the four and five flavor numbe…

Quantum chromodynamicsPhysicsGauge bosonParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHadronElectroweak interactionGeneral Physics and Astronomy7. Clean energy01 natural sciencesCross section (physics)Pair production0103 physical sciencesHigh Energy Physics::ExperimentPerturbation theory (quantum mechanics)010306 general physicsPhysical Review Letters
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Transverse-momentum resummation for vector-boson pair production at NNLL+NNLO

2015

We consider the transverse-momentum ($p_T$) distribution of $ZZ$ and $W^+W^-$ boson pairs produced in hadron collisions. At small $p_T$, the logarithmically enhanced contributions due to multiple soft-gluon emission are resummed to all orders in QCD perturbation theory. At intermediate and large values of $p_T$, we consistently combine resummation with the known fixed-order results. We exploit the most advanced perturbative information that is available at present: next-to-next-to-leading logarithmic resummation combined with the next-to-next-to-leading fixed-order calculation. After integration over $p_T$, we recover the known next-to-next-to-leading order result for the inclusive cross se…

Quantum chromodynamicsPhysicsParticle physicsNuclear and High Energy PhysicsLarge Hadron Collider530 PhysicsHadronHigh Energy Physics::PhenomenologyFOS: Physical sciences10192 Physics InstituteVector bosonHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyPair productionHigh Energy Physics - Phenomenology (hep-ph)RapidityHigh Energy Physics::ExperimentPerturbation theory (quantum mechanics)Resummation3106 Nuclear and High Energy PhysicsNuclear Experiment
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NLO QCD+EW predictions for V+jets including off-shell vector-boson decays and multijet merging

2016

We present next-to-leading order (NLO) predictions including QCD and electroweak (EW) corrections for the production and decay of off-shell electroweak vector bosons in association with up to two jets at the 13 TeV LHC. All possible dilepton final states with zero, one or two charged leptons that can arise from off-shell W and Z bosons or photons are considered. All predictions are obtained using the automated implementation of NLO QCD+EW corrections in the OpenLoops matrix-element generator combined with the Munich and Sherpa Monte Carlo frameworks. Electroweak corrections play an especially important role in the context of BSM searches, due to the presence of large EW Sudakov logarithms a…

Nuclear and High Energy PhysicsParticle physics530 PhysicsFOS: Physical sciencesContext (language use)10192 Physics InstituteAstrophysics::Cosmology and Extragalactic AstrophysicsJet (particle physics)01 natural sciencesVector bosonHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences3106 Nuclear and High Energy Physics010306 general physicsNuclear ExperimentQCBosonQuantum chromodynamicsPhysics010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyW′ and Z′ bosonsHigh Energy Physics::ExperimentLepton
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$W^{+}W^{-}$ production at the LHC: fiducial cross sections and distributions in NNLO QCD

2016

We consider QCD radiative corrections to $W^+W^-$ production at the LHC and present the first fully differential predictions for this process at next-to-next-to-leading order (NNLO) in perturbation theory. Our computation consistently includes the leptonic decays of the $W$ bosons, taking into account spin correlations, off-shell effects and non-resonant contributions. Detailed predictions are presented for the different-flavour channel $pp\to\mu^+e^-\nu_\mu {\bar \nu}_e+X$ at $\sqrt{s}=8$ and $13$ TeV. In particular, we discuss fiducial cross sections and distributions in the presence of standard selection cuts used in experimental $W^+W^-$ and $H\to W^+W^-$ analyses at the LHC. The inclus…

Nuclear and High Energy Physicsleptonic decay010308 nuclear & particles physics530 Physicsoff-shell [effect]High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciences10192 Physics Institute01 natural sciences2 [higher-order]High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CERN LHC Collcorrelation [spin]radiative correction [quantum chromodynamics]0103 physical sciencesddc:530High Energy Physics::Experimentexpansion 1/N3106 Nuclear and High Energy Physics010306 general physicsperturbation theoryJHEP
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