Search results for "Qcd"

showing 10 items of 614 documents

Correlators of left charges and weak operators in finite volume chiral perturbation theory

2002

We compute the two-point correlator between left-handed flavour charges, and the three-point correlator between two left-handed charges and one strangeness violating \Delta I=3/2 weak operator, at next-to-leading order in finite volume SU(3)_L x SU(3)_R chiral perturbation theory, in the so-called epsilon-regime. Matching these results with the corresponding lattice measurements would in principle allow to extract the pion decay constant F, and the effective chiral theory parameter g_27, which determines the \Delta I = 3/2 amplitude of the weak decays K to \pi\pi as well as the kaon mixing parameter B_K in the chiral limit. We repeat the calculations in the replica formulation of quenched c…

PhysicsNuclear and High Energy PhysicsChiral perturbation theoryFinite volume methodHigh Energy Physics::LatticeFlavourHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesFísicaParticle Physics - LatticeStrangenessweak decaysOperator (computer programming)AmplitudeHigh Energy Physics - Latticechiral Lagrangianslattice QCDLattice (order)kaon physicsPion decay constantMathematical physics
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Meson resonances, large N_c and chiral symmetry

2003

14 páginas, 2 tablas.-- arXiv:hep-ph/0305311v1

PhysicsNuclear and High Energy PhysicsChiral symmetryParticle physicsMesonHigh Energy Physics::LatticeScalar (mathematics)High Energy Physics::PhenomenologyFOS: Physical sciencesFísica1/N ExpansionMass matrixQCDHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Mass spectrumHigh Energy Physics::ExperimentLimit (mathematics)Chiral lagrangians
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A new representation of the Adler function for lattice QCD

2013

We address several aspects of lattice QCD calculations of the hadronic vacuum polarization and the associated Adler function. We implement a representation derived previously which allows one to access these phenomenologically important functions for a continuous set of virtualities, irrespective of the flavor structure of the current. Secondly we present a theoretical analysis of the finite-size effects on our particular representation of the Adler function, based on the operator product expansion at large momenta and on the spectral representation of the Euclidean correlator at small momenta. Finally, an analysis of the flavor structure of the electromagnetic current correlator is perform…

PhysicsNuclear and High Energy PhysicsCurrent (mathematics)DiagramLattice field theoryHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyRepresentation (systemics)FOS: Physical sciencesFunction (mathematics)Lattice QCDHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeVacuum polarizationOperator product expansionMathematical physics
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Extraction of K --> pi pi matrix elements with Wilson fermions

2001

We present the status of a lattice calculation for the K-->pipi matrix elements of the (delta S=1) effective weak Hamiltonian, directly with two pion in the final state. We study the energy shift of two pion in a finite volume both in the I=0 and I=2 channels. We explain a method to avoid the Goldstone pole contamination in the computation of renormalization constants for (delta I=3/2) operators. Finally we show some preliminary results for the matrix elements of (delta I=1/2) operators. Our quenched simulation is done at beta=6.0, with Wilson fermions, on a (24^3 X 64) lattice.

PhysicsNuclear and High Energy PhysicsFinite volume methodComputationHigh Energy Physics::LatticeFermionAtomic and Molecular Physics and OpticsRenormalizationFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIsymbols.namesakePionHigh Energy Physics - Latticelattice qcdLattice (order)visual_artvisual_art.visual_art_mediumsymbolsFísica nuclearHamiltonian (quantum mechanics)GoldstoneMathematical physics
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Predictions for cold nuclear matter effects in p+Pb collisions at sNN=8.16 TeV

2018

Predictions for cold nuclear matter effects on charged hadrons, identified light hadrons, quarkonium and heavy flavor hadrons, Drell–Yan dileptons, jets, photons, gauge bosons and top quark pairs produced in p +Pb collisions at sNN=8.16 TeV are compiled and, where possible, compared to each other. Predictions of the normalized ratios of p +Pb to p+p cross sections are also presented for most of the observables, providing new insights into the expected role of cold nuclear matter effects. In particular, the role of nuclear parton distribution functions on particle production can now be probed over a wider range of phase space than ever before.

PhysicsNuclear and High Energy PhysicsGauge bosonTop quark010308 nuclear & particles physicsNuclear TheoryHigh Energy Physics::PhenomenologyHadronDrell–Yan processPerturbative QCDPartonNuclear matterQuarkonium01 natural sciencesNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsNuclear Physics A
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Covariant approximation averaging

2015

We present a new class of statistical error reduction techniques for Monte-Carlo simulations. Using covariant symmetries, we show that correlation functions can be constructed from inexpensive approximations without introducing any systematic bias in the final result. We introduce a new class of covariant approximation averaging techniques, known as all-mode averaging (AMA), in which the approximation takes account of contributions of all eigenmodes through the inverse of the Dirac operator computed from the conjugate gradient method with a relaxed stopping condition. In this paper we compare the performance and computational cost of our new method with traditional methods using correlation…

PhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeMonte Carlo methodLattice field theoryHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesLattice QCDDirac operatorsymbols.namesakeHigh Energy Physics - LatticeConjugate gradient methodLattice gauge theoryQuantum mechanicssymbolsCovariant transformationVector mesonMathematical physics
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Instantons and eta meson production near threshold in NN collisions

1999

An enhancement for the $\eta$ production in proton-neutron collisions as compared with that in proton-proton scattering has been recently observed. We present a calculation for the production cross section, in proton-neutron collisions near threshold, within instanton model for the QCD vacuum and show that a specific flavor dependent nonperturbative quark-gluon interaction related to instantons is able to explain the observed enhancement.

PhysicsNuclear and High Energy PhysicsInstantonParticle physicsScatteringHigh Energy Physics::LatticeEta mesonQCD vacuumNuclear TheoryHigh Energy Physics::PhenomenologyFísicaCross section (physics)Near thresholdHigh Energy Physics - PhenomenologyProduction (computer science)High Energy Physics::ExperimentNuclear Experiment
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A measurement of the ratio of the W and Z cross sections with exactly one associated jet in pp collisions at with ATLAS

2012

The ratio of production cross sections of the W and Z bosons with exactly one associated jet is presented as a function of jet transverse momentum threshold. The measurement has been designed to ma ...

PhysicsNuclear and High Energy PhysicsJet (fluid)Particle physics010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaPerturbative QCDFunction (mathematics)01 natural sciencesStandard ModelNuclear physicsmedicine.anatomical_structureAtlas (anatomy)W and Z bosons0103 physical sciencesTransverse momentummedicineHigh Energy Physics::Experiment010306 general physics
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Measurement of the differential cross section of photon plus jet production inpp¯collisions ats=1.96  TeV

2013

We study the process of associated photon and jet production, p (p) over bar -> gamma + jet + X, using 8.7 fb(-1) of integrated luminosity collected by the D0 detector at the Fermilab Tevatron Collider at a center-of-mass energy root s = 1.96 TeV. Photons are reconstructed with rapidity vertical bar y(gamma)vertical bar 20 GeV. The highest-p(T) jet is required to be in one of four rapidity regions up to vertical bar y(jet)vertical bar 0) and opposite signs (y(gamma)y(jet) <= 0) of photon and jet rapidities. We compare the measured triple-differential cross sections, d(3)sigma/dp(T)(gamma)dy(gamma)dy(jet), to next-to-leading order (NLO) perturbative QCD calculations using different sets of p…

PhysicsNuclear and High Energy PhysicsJet (fluid)Particle physicsLarge Hadron Collider010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyTevatronPerturbative QCDPartonHERA01 natural scienceslaw.inventionNuclear physicslaw0103 physical sciencesHigh Energy Physics::ExperimentRapidity010306 general physicsColliderPhysical Review D
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Precision measurements of B(D+→μ+νμ), the pseudoscalar decay constant fD+, and the quark mixing matrix element |Vcd|

2014

We report a measurement of the branching fraction B(D+ -> mu(+)nu(mu)) = [3.71 +/- 0.19(stat) +/- 0.06(sys)] x 10(-4) based on 2.92 fb(-1) of data accumulated at root s = 3.773 GeV with the BESIII detector at the BEPCII collider. This measurement, in conjunction with the Cabibbo-Kobayashi-Maskawa matrix element vertical bar V-cd vertical bar determined from a global Standard Model fit, implies a value for the weak decay constant f(D+) = (203.2 +/- 5.3 +/- 1.8) MeV. Additionally, using this branching fraction measurement together with a lattice QCD prediction for f(D+), we find vertical bar V-cd vertical bar 0.2210 +/- 0.0058 +/- 0.0047. In either case, these are the most precise results for…

PhysicsNuclear and High Energy PhysicsMeson010308 nuclear & particles physicsBranching fractionCabibbo–Kobayashi–Maskawa matrixElectron–positron annihilationLattice QCD01 natural sciencesStandard ModelNuclear physicsPseudoscalar0103 physical sciencesExponential decay010306 general physics
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