Search results for "perturbative QCD"

showing 10 items of 174 documents

Measurements of differential cross sections of Z/γ∗+jets+X events in pp¯ collisions at s=1.96 TeV

2009

We present cross section measurements for Z/gamma* + jets + X production, differential in the transverse momenta of the three leading jets. The data sample was collected with the DO detector at the Fermilab Tevatron p (p) over bar collider at a center-of-mass energy of 1.96 TeV and corresponds to an integrated luminosity of 1 fb(-1). Leading and next-to-leading order perturbative QCD predictions are compared with the measurements. and agreement is found within the theoretical and experimental uncertainties. We also make comparisons with the predictions of four event generators. Two parton-shower-based generators show significant shape and normalization differences with respect to the data. …

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsTevatronPerturbative QCD7. Clean energy01 natural scienceslaw.inventionlaw0103 physical sciencesHigh Energy Physics::ExperimentFermilab010306 general physicsColliderParton showerEvent (particle physics)Physics Letters B
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Measurement of the ratio of three-jet to two-jet cross sections in pp¯ collisions at s=1.96 TeV

2013

We present a measurement of the ratio of multijet cross sections in pp-bar collisions at sqrt(s) = 1.96 TeV at the Fermilab Tevatron Collider. The measurement is based on a data set corresponding to an integrated luminosity of 0.7 fb-1 collected with the D0 detector. The ratio of the inclusive three-jet to two-jet cross sections, R3/2, has been measured as a function of the jet transverse momenta. The data are compared to QCD predictions in different approximations. Popular tunes of the PYTHIA event generator do not agree with the data, while SHERPA provides a reasonable description of the data. A perturbative QCD prediction in next-to-leading order in the strong coupling constant, correcte…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsTevatronPerturbative QCDJet (particle physics)01 natural scienceslaw.inventionNuclear physicslaw0103 physical sciencesHigh Energy Physics::ExperimentFermilab010306 general physicsColliderEvent generatorPhysics Letters B
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B-meson decays toη′ρ,η′f0, andη′K*

2010

We present measurements of B-meson decays to the final states η′ρ, η′f_0, and η′K*, where K* stands for a vector, scalar, or tensor strange meson. We observe a significant signal or evidence for η′ρ^+ and all the η′K* channels. We also measure, where applicable, the charge asymmetries, finding results consistent with no direct CP violation in all cases. The measurements are performed on a data sample consisting of 467 × 10^6 BB(overbar) pairs, collected with the BABAR detector at the PEP-II e^+e^- collider at the SLAC National Accelerator Laboratory. Our results favor the theoretical predictions from perturbative QCD and QCD factorization and we observe an enhancement of the tensor K*_2(143…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsMeson010308 nuclear & particles physicsScalar (mathematics)Perturbative QCDElementary particle01 natural sciencesNuclear physics0103 physical sciencesCP violationHigh Energy Physics::ExperimentB mesonTensor010306 general physicsPhysical Review D
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Hadronic contribution to the muong−2factor: A theoretical determination

2012

The leading-order hadronic contribution to the muon $g\ensuremath{-}2$, ${a}_{\ensuremath{\mu}}^{\mathrm{HAD}}$, is determined entirely from theory using an approach based on Cauchy's theorem in the complex squared energy $s$-plane. This is possible after fitting the integration kernel in ${a}_{\ensuremath{\mu}}^{\mathrm{HAD}}$ with a simpler function of $s$. The integral determining ${a}_{\ensuremath{\mu}}^{\mathrm{HAD}}$ in the light-quark region is then split into a low-energy and a high-energy part, the latter given by perturbative QCD (PQCD). The low energy integral involving the fit function to the integration kernel is determined by derivatives of the vector correlator at the origin,…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsMuonChiral perturbation theoryHigh Energy Physics::PhenomenologyHadronPerturbative QCDHigh Energy Physics::ExperimentLattice QCDRealization (systems)Energy (signal processing)Physical Review D
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Measurement of the transverse momentum distribution of Z/γ⁎ bosons in proton–proton collisions at s=7 TeV with the ATLAS detector

2011

A measurement of the Z/gamma* transverse momentum (p(T)(Z)) distribution in proton-proton collisions at root s = 7 TeV is presented using Z/gamma* -> e(+)e(-) and Z/gamma* -> mu(+)mu(-) decay ...

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsMuonProton010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryMonte Carlo methodPerturbative QCDElectron01 natural sciencesNuclear physicsmedicine.anatomical_structureAtlas (anatomy)0103 physical sciencesmedicinePhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsBosonPhysics Letters B
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Direct photon production in Pb–Pb collisions atsNN=2.76 TeV

2016

Direct photon production at mid-rapidity in Pb–Pb collisions at √sNN = 2.76 TeV was studied in the transverse momentum range 0.9<pT<14 GeV/c. Photons were detected with the highly segmented electromagnetic calorimeter PHOS and via conversions in the ALICE detector material with the e+e− pair reconstructed in the central tracking system. The results of the two methods were combined and direct photon spectra were measured for the 0–20%, 20–40%, and 40–80% centrality classes. For all three classes, agreement was found with perturbative QCD calculations for pT≳5 GeV/c. Direct photon spectra down to pT≈1 GeV/c could be extracted for the 20–40% and 0–20% centrality classes. The significance of th…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsPhoton010308 nuclear & particles physicsHadronBremsstrahlungPerturbative QCD01 natural sciencesParticle identificationNuclear physics0103 physical sciencesRapidityNuclear Experiment010306 general physicsGlauberPhysics Letters B
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Brodsky-Lepage-Mackenzie scale for the pion transition form factor

2002

The next-to-leading order (NLO) Brodsky-Lepage-Mackenzie (BLM) scale for the pion transition form factor is determined. To achieve that, a consistent calculation up to ${n}_{f}$-proportional next-to-next-to-leading order contributions to both the hard-scattering amplitude and the perturbatively calculable part of the pion distribution amplitude is performed. By combining and matching the results obtained for these two amplitudes, a proper cancellation of collinear singularities is established and the ${\ensuremath{\gamma}}_{5}$ ambiguity problem (related to the use of the dimensional regularization method) is resolved by using the naive-${\ensuremath{\gamma}}_{5}$ as well as the 't Hooft--V…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsPhysicsHigh Energy Physics::PhenomenologyForm factor (quantum field theory)Order (ring theory)Astronomy and AstrophysicsCoupling (probability)Distribution (mathematics)AmplitudePionFactorizationBLM; pion transition form factor; NNLO; perturbative QCD
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Charm quark mass determined from a pair of sum rules

2016

In this paper, we present preliminary results of the determination of the charm quark mass $\hat{m}_c$ from QCD sum rules of moments of the vector current correlator calculated in perturbative QCD at ${\cal O} (\hat \alpha_s^3)$. Self-consistency between two different sum rules allow to determine the continuum contribution to the moments without requiring experimental input, except for the charm resonances below the continuum threshold. The existing experimental data from the continuum region is used, then, to confront the theoretical determination and reassess the theoretic uncertainty.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsQCD sum rulesCurrent (mathematics)010308 nuclear & particles physicsContinuum (topology)High Energy Physics::PhenomenologyGeneral Physics and AstronomyPerturbative QCDFOS: Physical sciencesAstronomy and Astrophysics01 natural sciencesCharm quarkHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::ExperimentCharm (quantum number)Current vector010306 general physics
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In-medium jet shape from energy collimation in parton showers: Comparison with CMS PbPb data at 2.76 TeV

2014

We present the medium-modified energy collimation in the leading-logarithmic approximation (LLA) and next-to-leading-logarithmic approximation (NLLA) of QCD. As a consequence of more accurate kinematic considerations in the argument of the Dokshitzer-Gribov-Lipatov-Altarelli-Parisi (DGLAP) fragmentation functions (FFs) we find a new NLLA correction ${\cal O}(\alpha_s)$ which accounts for the scaling violation of DGLAP FFs at small $x$. The jet shape is derived from the energy collimation within the same approximations and we also compare our calculations for the energy collimation with the event generators Pythia 6 and YaJEM for the first time in this paper. The modification of jets by the …

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsta114Astrophysics::High Energy Astrophysical PhenomenaPerturbative QCDFOS: Physical sciencesPartonGluonHadronizationNuclear physicsHigh Energy Physics - PhenomenologyDGLAPHigh Energy Physics - Phenomenology (hep-ph)Quark–gluon plasmaHigh Energy Physics::ExperimentScaling
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Measurement of the normalized Z/γ∗→μ+μ− transverse momentum distribution in pp¯ collisions at s=1.96 TeV

2010

We present a new measurement of the Z/gamma* transverse momentum distribution in the range 0-330 GeV, in proton-antiproton collisions at root s = 1.96 TeV. The measurement uses 0.97 fb(-1) of integrated luminosity recorded by the D0 experiment and is the first using the Z/gamma* -> mu(+)mu(-) + X channel at this center-of-mass energy. This is also the first measurement of the Z/gamma* transverse momentum distribution that presents the result at the level of particles entering the detector, minimizing dependence on theoretical models. As any momentum of the Z/gamma* in the plane transverse to the incoming beams must be balanced by some recoiling system, primarily the result of QCD radiation …

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsRange (particle radiation)Particle physicsLarge Hadron ColliderLuminosity (scattering theory)010308 nuclear & particles physicsHadronPerturbative QCD01 natural sciencesNuclear physicsMomentumTransverse plane0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysics Letters B
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