Search results for "FERMILAB"

showing 10 items of 248 documents

Measurements of inclusive W+jets production rates as a function of jet transverse momentum in pp¯ collisions at s=1.96 TeV

2011

This Letter describes measurements of inclusive W (--> e nu) + n jet cross sections (n = 1-4), presented as total inclusive cross sections and differentially in the nth jet transverse momentum. The measurements are made using data corresponding to an integrated luminosity of 4.2 fb-1 collected by the D0 detector at the Fermilab Tevatron Collider, and achieve considerably smaller uncertainties on W +jets production cross sections than previous measurements. The measurements are compared to next-to-leading order perturbative QCD (pQCD) calculations in the n =1-3 jet multiplicity bins and to leading order pQCD calculations in the 4-jet bin. The measurements are generally in agreement with pQCD…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsTevatronPerturbative QCD7. Clean energy01 natural sciencesBinNuclear physicsPhase space0103 physical sciencesHigh Energy Physics::ExperimentFermilabMultiplicity (chemistry)010306 general physicsN-jetPhysics Letters B
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Results from bottomonia production at the Tevatron and prospects for the LHC

2000

We extend our previous analysis on inclusive heavy quarkonia hadroproduction to the whole Upsilon(nS) (n=1,2,3) resonance family. We use a Monte Carlo framework with the colour-octet mechanism implemented in the PYTHIA event generator. We include in our study higher order QCD effects such as initial-state emission of gluons and Altarelli-Parisi evolution of final-state gluons. We extract some NRQCD colour-octet matrix elements relevant for Upsilon(nS) (n=1,2,3) hadroproduction from CDF data at the Fermilab Tevatron. Then we extrapolate to LHC energies to predict prompt bottomonia production rates. Finally, we examine the prospect to probe the gluon density in protons from heavy quarkonia in…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderHigh Energy Physics::LatticeMonte Carlo methodHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciencesFísicaResonance (particle physics)GluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentFermilabNuclear ExperimentParticle Physics - PhenomenologyEvent generator
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Measurement of the dijet invariant mass cross section in pp¯ collisions at s=1.96 TeV

2010

The inclusive dijet production double differential cross section as a function of the dijet invariant mass and of the largest absolute rapidity (y_{max}) of the two jets with the largest transverse momentum in an event is measured in proton anti-proton collisions at sqrt{s} = 1.96$ TeV using 0.7 fb^{-1} of data collected with the D0 detector at the Fermilab Tevatron Collider. The measurement is performed in six rapidity regions up to |y|=2.4. Next-to-leading order perturbative QCD predictions are found to be in agreement with the data.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsProton010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronPerturbative QCD01 natural scienceslaw.inventionNuclear physicslaw0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentInvariant massRapidityFermilabNuclear Experiment010306 general physicsColliderPhysics Letters B
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Determination of the pole and MS¯ masses of the top quark from the tt¯ cross section

2011

We use higher-order quantum chromodynamics calculations to extract the mass of the top quark from the ttbar cross section measured in the lepton+jets channel in ppbar collisions at sqrt(s)=1.96 TeV using 5.3 fb-1 of integrated luminosity collected by the D0 experiment at the Fermilab Tevatron Collider. The extracted top quark pole mass and MSbar mass are compared to the current Tevatron average top quark mass obtained from direct measurements.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsTop quarkParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyTevatronD0 experiment7. Clean energy01 natural sciencesBottom quarkNuclear physics0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentB mesonFermilab010306 general physicsPhysics Letters B
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Measurement of Inclusive Jet Cross Sections inZ/γ*(→e+e−)+jetsProduction inpp¯Collisions ats=1.96   TeV

2008

Inclusive jet cross sections in Z/{gamma}* events, with Z/{gamma}* decaying into an electron-positron pair, are measured as a function of jet transverse momentum and jet multiplicity in p{bar p} collisions at {radical}s - 1.96 TeV with the upgraded Collider Detector at Fermilab in Run II, based on an integrated luminosity of 1.7 fb{sup -1}. The measurements cover the rapidity region |y{sup jet}| 30 GeV/c. Next-to-leading order perturbative QCD predictions are in good agreement with the measured cross sections.

PhysicsQuantum chromodynamicsParticle physicsAnnihilation010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaGeneral Physics and AstronomyPerturbative QCDElectron01 natural sciences7. Clean energyNuclear physicsPair production0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentRapidityMultiplicity (chemistry)010306 general physicsCollider Detector at FermilabPhysical Review Letters
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Review of Lattice QCD Studies of Hadronic Vacuum Polarization Contribution to Muon g-2

2019

Lattice QCD (LQCD) studies for the hadron vacuum polarization (HVP) and its contribution to the muon anomalous magnetic moment (muon g-2) are reviewed. There currently exists more than 3-sigma deviations in the muon g-2 between the BNL experiment with 0.5 ppm precision and the Standard Model (SM) predictions, where the latter relies on the QCD dispersion relation for the HVP. The LQCD provides an independent crosscheck of the dispersive approaches and important indications for assessing the SM prediction with measurements at ongoing/forthcoming experiments at Fermilab/J-PARC (0.14/0.1 ppm precision). The LQCD has made significant progress, in particular, in the long distance and finite volu…

PhysicsQuantum chromodynamicsParticle physicsMuonAnomalous magnetic dipole momentPhysics beyond the Standard ModelHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesLattice QCDHigh Energy Physics - LatticeIsospinHigh Energy Physics::ExperimentFermilabVacuum polarization
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Ratio of Isolated Photon Cross Sections in pp¯ Collisions at √s=630 and 1800 GeV

2001

The inclusive cross section for production of isolated photons has been measured in p (p) over bar collisions at roots = 630 GeV with the DO detector at the Fermilab Tevatron Collider. The photons span a transverse energy (E-T) range from 7-49 GeV and have pseudorapidity \eta\ s = 1800 GeV to form a ratio of the cross sections. Comparison of next-to-leading-order QCD with the measured cross section at 630 GeV and the ratio of cross sections show satisfactory agreement in most of the E-T range.

PhysicsQuantum chromodynamicsParticle physicsPhoton010308 nuclear & particles physicsTevatronGeneral Physics and Astronomy7. Clean energy01 natural scienceslaw.inventionNuclear physicsCross section (physics)lawPseudorapidity0103 physical sciencesHigh Energy Physics::ExperimentFermilabNuclear Experiment010306 general physicsColliderBar (unit)Physical Review Letters
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Charge asymmetry of heavy quarks at hadron colliders

1998

A sizeable difference in the differential production cross section of top and antitop quarks, respectively, is predicted for hadronically produced heavy quarks. It is of order $\alpha_s$ and arises from the interference between charge odd and even amplitudes respectively. For the TEVATRON it amounts up to 15\% for the differential distribution in suitable chosen kinematical regions. The resulting integrated forward-backward asymmetry of 4--5\% could be measured in the next round of experiments. At the LHC the asymmetry can be studied by selecting appropriately chosen kinematical regions. Furthermore, a slight preference at LHC for centrally produced antitop is predicted, with top quarks mor…

PhysicsQuantum chromodynamicsQuarkNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderHigh Energy Physics::Latticemedia_common.quotation_subjectHadronHigh Energy Physics::PhenomenologyTevatronFísicaOrder (ring theory)FOS: Physical sciencesAsymmetryNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentFermilabmedia_common
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Measurement of spin correlation in tt¯ production using dilepton final states

2011

We measure the correlation between the spin of the top quark and the spin of the anti-top quark in (ttbar -> W+ W- b bbar -> l+ nu b l- nubar bbar) final states produced in ppbar collisions at a center of mass energy sqrt(s)=1.96 TeV, where l is an electron or muon. The data correspond to an integrated luminosity of 5.4 fb-1 and were collected with the D0 detector at the Fermilab Tevatron collider. The correlation is extracted from the angles of the two leptons in the t and tbar rest frames, yielding a correlation strength C= 0.10^{+0.45}_{-0.45}, in agreement with the NLO QCD prediction within two standard deviations, but also in agreement with the no correlation hypothesis.

PhysicsQuantum chromodynamicsQuarkNuclear and High Energy PhysicsParticle physicsTop quarkMuonPhysics::Instrumentation and Detectors010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatron01 natural sciencesNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentFermilabCenter of mass010306 general physicsLeptonPhysics Letters B
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Search for scalar bottom quarks and third-generation leptoquarks in pp¯ collisions at s=1.96 TeV

2010

We report the results of a search for pair production of scalar bottom quarks ((b) over bar (1)) and scalar third-generation leptoquarks (LQ(3)) in 5.2 fb(-1) of p (p) over bar collisions at the D0 experiment of the Fermilab Tevatron Collider. Scalar bottom quarks are assumed to decay to a neutralino ((chi) over bar (1)(0)) and a b quark, and we set 95% C.L. lower limits on their production in the (m((b) over bar1), m((chi) over bar 10)) mass plane such as m((b) over bar1) > 247 GeV for m( 10) = 0 and m((chi) over bar 10) > 110 GeV for 160 m(<(b) over bar1) < 200 GeV. The leptoquarks are assumed to decay to a tau neutrino and a b quark, and we set a 95% C.L. lower limit of 247 GeV on the ma…

PhysicsQuarkNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyScalar (mathematics)Tevatron01 natural sciences7. Clean energyBottom quarkNuclear physicsTau neutrino0103 physical sciencesNeutralinoHigh Energy Physics::ExperimentLeptoquarkFermilab010306 general physicsPhysics Letters B
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