Search results for "Production"

showing 10 items of 7600 documents

Comprehensive measurements oft-channel single top-quark production cross sections ats=7  TeVwith the ATLAS detector

2014

This article presents measurements of the t-channel single top-quark ((t) over bart) and top-antiquark (_ t) total production cross sections sdtq_ and sd _ tq_, their ratio Rt sdtq_= sd _ tq_, and a measurement of the inclusive production cross section sdtq _ _ tq_ in proton-proton collisions at ffiffiffi ps = 7 TeV at the LHC. Differential cross sections for the tq and _ tq processes are measured as a function of the transverse momentum and the absolute value of the rapidity of t and _ t, respectively. The analyzed data set was recorded with the ATLAS detector and corresponds to an integrated luminosity of 4.59 fb-1. Selected events contain one charged lepton, large missing transverse mome…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsTop quarkParticle physics010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrix01 natural sciencesStandard ModelNuclear physicsmedicine.anatomical_structurePair productionAtlas (anatomy)0103 physical sciencesmedicineRapidity010306 general physicsLeptonPhysical Review D
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Dependence of the tt¯ production cross section on the transverse momentum of the top quark

2010

We present a measurement of the differential cross section for $t\bar{t}$ events produced in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV as a function of the transverse momentum ($p_T$) of the top quark. The selected events contain a high-$p_T$ lepton ($\ell$), four or more jets, and a large imbalance in $p_T$, and correspond to 1 fb${}^{-1}$ of integrated luminosity recorded with the D0 detector. Each event must have at least one candidate for a $b$ jet. Objects in the event are associated through a constrained kinematic fit to the $t\bar{t}\to WbW\bar{b} \to \ell\nu b q\bar{q}'\bar{b}$ process. Results from next-to-leading-order perturbative QCD calculations agree with the measured diffe…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsTop quarkParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsBar (music)High Energy Physics::PhenomenologyPerturbative QCDJet (particle physics)01 natural sciencesNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)010306 general physicsLeptonPhysics Letters B
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Combination oftt¯cross section measurements and constraints on the mass of the top quark and its decays into charged Higgs bosons

2009

We combine measurements of the top quark pair production cross section in p (p) over bar collisions in the l + jets, ll, and tau l final states ( where l is an electron or muon) at a center of mass energy of root s = 1.96 TeV in 1 fb(-1) of data collected with the D0 detector. For a top quark mass of 170 GeV/c(2), we obtain sigma(t (t) over bar) = 8.18(-0.87)(+0.98) pb in agreement with the theoretical prediction. Based on predictions from higher order quantum chromodynamics, we extract a mass for the top quark from the combined t (t) over bar cross section, consistent with the world average of the top quark mass. In addition, the ratios of t (t) over bar cross sections in different final s…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsTop quarkParticle physicsMuon010308 nuclear & particles physicsBranching fractionHigh Energy Physics::Phenomenology7. Clean energy01 natural sciencesNuclear physicsParticle decayPair production0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsBosonPhysical Review D
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Measurement of the tt¯ production cross section and top quark mass extraction using dilepton events in pp¯ collisions

2009

We present a measurement of the top quark pair production cross section in p (p) over bar collisions at root s = 1.96 TeV using approximately 1 fb(-1) collected with the DO detector. We consider decay channels containing two high p(T) charged leptons where one lepton is identified as an electron or a muon while the other lepton can be an electron, a muon or a hadronically decaying tau lepton. For a mass of the top quark of 170 GeV, the measured cross section is 7.5(-1.0)(+1.0)(stat)(-0.6)(+0.7)(syst)(-0.5)(+0.6)(lumi) pb. Using l tau events only, we measure: sigma(t (t) over bar) x B(t (t) over bar -> l tau b (b) over bar) = 0.13(-0.08)(+0.09)(stat)(-0.06)(+0.06)(syst)(-0.02)(+0.02)(lumi) p…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsTop quarkParticle physicsMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyElectron01 natural sciences7. Clean energyNuclear physicsCross section (physics)Pair production0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsLeptonBar (unit)Physics Letters B
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Inclusive dijet photoproduction in ultraperipheral heavy ion collisions at the CERN Large Hadron Collider in next-to-leading order QCD

2019

We compute the cross section of inclusive dijet photoproduction in ultraperipheral Pb-Pb collisions at the CERN Large Hadron Collider using next-to-leading order perturbative QCD. We demonstrate that our theoretical calculations provide a good description of various kinematic distributions measured by the ATLAS Collaboration. We find that the calculated dijet photoproduction cross section is sensitive to nuclear modifications of parton distribution functions (PDFs) at the level of 10% to 20%. Hence, this process can be used to reduce uncertainties in the determination of these nuclear PDFs, whose current magnitude is comparable to the size of the calculated nuclear modifications of the dije…

Quantum chromodynamicsPhysicsPB-PB COLLISIONSParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyNuclear TheoryPerturbative QCDPartonhiukkasfysiikkaJ/PSI PHOTOPRODUCTION01 natural sciences114 Physical sciencesCROSS-SECTIONSPHYSICSDistribution functionHERA DIRECTRHO0103 physical sciencesHeavy ionHigh Energy Physics::Experiment010306 general physicsNuclear Experiment
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WZ Production in Association with Two Jets at Next-to-Leading Order in QCD

2013

We report on the calculation of W-+/- Zjj production with leptonic decays at hadron-hadron colliders at next-to-leading order in QCD. These processes are important both to test the quartic gauge couplings of the standard model and because they constitute relevant backgrounds to beyond standard model physics searches. Our results show that the next-to-leading order corrections reduce significantly the scale uncertainties and have a nontrivial phase space dependence.

Quantum chromodynamicsPhysicsParticle physics010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyOrder (ring theory)Gauge (firearms)NLO QCD01 natural sciencesStandard ModelPhase spaceQuartic function0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)010306 general physicsHadron colliders
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Measurement of the Shape of the Boson-Transverse Momentum Distribution inpp¯→Z/γ*→e+e−+XEvents Produced ats=1.96  TeV

2008

We present a measurement of the shape of the Z/gamma* boson transverse momentum (q(T)) distribution in p (p) over bar -> Z/gamma(*)-> e(+)e(-)+X events at a center-of-mass energy of 1.96 TeV using 0.98 fb(-1) of data collected with the D0 detector at the Fermilab Tevatron collider. The data are found to be consistent with the resummation prediction at low q(T), but above the perturbative QCD calculation in the region of q(T)> 30 GeV/c. Using events with q(T)< 30 GeV/c, we extract the value of g(2), one of the nonperturbative parameters for the resummation calculation. Data at large boson rapidity y are compared with the prediction of resummation and with alternative models that employ a res…

Quantum chromodynamicsPhysicsParticle physicsAnnihilation010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronForm factor (quantum field theory)General Physics and AstronomyPerturbative QCD01 natural sciencesNuclear physicsPair production0103 physical sciencesHigh Energy Physics::ExperimentResummation010306 general physicsBosonPhysical Review Letters
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Heavy-flavour production in the SACOT-mT scheme

2019

The hadroproduction of heavy-flavoured mesons has recently attracted a growing interest e.g. within the people involved in global analysis of proton and nuclear parton distribution functions, saturation physics, and physics of cosmic rays. In particular, the D- and B-meson measurements of LHCb at forward direction are sensitive to gluon dynamics at small $x$ and are one of the few perturbative small-$x$ probes before the next generation deep-inelastic-scattering experiments. In this talk, we will concentrate on the collinear-factorization approach to inclusive D-meson production and describe a novel implementation --- SACOT-$m_{\rm T}$ --- of the general-mass variable flavour number scheme …

Quantum chromodynamicsPhysicsParticle physicsDistribution functionMesonProtonHigh Energy Physics::PhenomenologySaturation (graph theory)High Energy Physics::ExperimentProduction (computer science)PartonhiukkasfysiikkaGluonProceedings of International Conference on Hard and Electromagnetic Probes of High-Energy Nuclear Collisions — PoS(HardProbes2018)
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W+W− production at high transverse momenta beyond NLO

2014

Pair production of W gauge bosons is an important process at the LHC entering many experimental analyses, both as background in new-physics searches or Higgs measurements and as signal in precision studies and tests of the Standard Model. Therefore, accurate predictions for this class of processes are of great interest in order to exploit the full potential of LHC measurements. We use the LoopSim method to combine NLO QCD results for WW and WW + jet, as well as the loop-squared gluon-fusion contribution, to obtain approximate NNLO predictions for WW production. The cross sections are calculated with VBFNLO and include leptonic decays of the W bosons as well as finite-width and off-shell eff…

Quantum chromodynamicsPhysicsParticle physicsGauge bosonNuclear and High Energy PhysicsLarge Hadron ColliderPhysicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFOS: Physical sciencesStandard ModelNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Pair productionHiggs bosonddc:530High Energy Physics::ExperimentBosonNuclear Physics B
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Two-loop divergences of scattering amplitudes with massive partons

2009

We complete the study of two-loop infrared singularities of scattering amplitudes with an arbitrary number of massive and massless partons in non-abelian gauge theories. To this end, we calculate the universal functions F_1 and f_2, which completely specify the structure of three-parton correlations in the soft anomalous-dimension matrix, at two-loop order in closed analytic form. Both functions are found to be suppressed like O(m^4/s^2) in the limit of small parton masses, in accordance with mass factorization theorems proposed in the literature. On the other hand, they are unsuppressed and diverge logarithmically near the threshold for pair production of two heavy particles. As an applica…

Quantum chromodynamicsPhysicsParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesGeneral Physics and AstronomyPartonScattering amplitudeMassless particleMatrix (mathematics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Pair productionFactorizationQuantum field theory
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