Search results for "QCD Phenomenology"

showing 5 items of 15 documents

Heavy quark impact factor in kT-factorization

2013

We present the calculation of the finite part of the heavy quark impact factor at next-to-leading logarithmic accuracy in a form suitable for phenomenological studies such as the calculation of the cross-section for single bottom quark production at the LHC within the kT-factorization scheme.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderLogarithm010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesQCD Phenomenology01 natural sciencesBottom quarkHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)FactorizationNLO Computations0103 physical sciences010306 general physics
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Approximate NNLO predictions for the stop-pair production cross section at the LHC

2013

If the minimal supersymmetric standard model at scales of around 1 TeV is realized in nature, the total top-squark pair production cross section should be measurable at the CERN Large Hadron Collider. In this work we present precise predictions for this observable, which are based upon approximate NNLO formulas obtained using soft-collinear effective theory methods.

PhysicsWork (thermodynamics)Particle physicsNuclear and High Energy PhysicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesObservableQCD Phenomenology01 natural sciences3. Good healthHigh Energy Physics - PhenomenologyCross section (physics)High Energy Physics - Phenomenology (hep-ph)Pair productionSupersymmetry PhenomenologyQCD Phenomenology; Supersymmetry Phenomenology0103 physical sciencesEffective field theoryHigh Energy Physics::Experiment010306 general physicsMinimal Supersymmetric Standard Model
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Large Effects from Small QCD Instantons: Making Soft Bombs at Hadron Colliders

2020

It is a common belief that the last missing piece of the Standard Model of particles physics was found with the discovery of the Higgs boson at the Large Hadron Collider. However, there remains a major prediction of quantum tunnelling processes mediated by instanton solutions in the Yang-Mills theory, that is still untested in the Standard Model. The direct experimental observation of instanton-induced processes, which are a consequence of the non-trivial vacuum structure of the Standard Model and of quantum tunnelling in QFT, would be a major breakthrough in modern particle physics. In this paper, we present for the first time a full calculation of QCD instanton-induced processes in proton…

Quantum chromodynamicsPhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsInstantonLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::LatticeHadronHigh Energy Physics::PhenomenologyFOS: Physical sciencesQCD Phenomenology01 natural sciencesStandard ModelGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)0103 physical sciencesHiggs bosonlcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEvent generator
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B-meson hadroproduction in the SACOT-mT scheme

2023

We apply the SACOT-mT general-mass variable flavour number scheme (GM-VFNS) to the inclusive B-meson production in hadronic collisions at next-to-leading order in perturbative Quantum Chromodynamics. In the GM-VFNS approach one matches the fixed-order heavy-quark production cross sections, accurate at low transverse momentum (pT), with the zero-mass cross sections, accurate at high pT. The physics idea of the SACOT-mT scheme is to do this by accounting for the finite momentum transfer required to create a heavy quark-antiquark pair throughout the calculation. We compare our results with the latest LHC data from proton-proton and proton-lead collisions finding a very good agreement within th…

bottom quarksParton distributionsspecific QCD phenomenology
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Spatially dependent parton distribution functions and hard processes in nuclear collisions

2014

hadron productionparton distribution functionsHeavy ion phenomenologythermal photonsNuclear PDFsHard processestermiset fotonitnuclear collisionsfragmentation functionsDirect photonsQCD phenomenologypartonijakaumatfragmentaatiofunktiotydintörmäyksetForward rapiditiesteoreettinen fysiikkaProton+nucleus collisionshadronituotto
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