Search results for "lattice [space-time]"

showing 10 items of 692 documents

Low-energy couplings of QCD from current correlators near the chiral limit

2004

We investigate a new numerical procedure to compute fermionic correlation functions at very small quark masses. Large statistical fluctuations, due to the presence of local ``bumps'' in the wave functions associated with the low-lying eigenmodes of the Dirac operator, are reduced by an exact low-mode averaging. To demonstrate the feasibility of the technique, we compute the two-point correlator of the left-handed vector current with Neuberger fermions in the quenched approximation, for lattices with a linear extent of L~1.5 fm, a lattice spacing a~0.09 fm, and quark masses down to the epsilon-regime. By matching the results with the corresponding (quenched) chiral perturbation theory expres…

QuarkNuclear and High Energy PhysicsChiral perturbation theoryCurrent (mathematics)High Energy Physics::LatticeFOS: Physical sciencesQuenched approximationStatistical fluctuationsDirac operatorsymbols.namesakechiral Lagrangianslattice QCDHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Latticelattice gauge field theoriesPhysicsQuantum chromodynamicsHigh Energy Physics - Lattice (hep-lat)FísicaFermionQCDFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - PhenomenologyLattice gauge theoryQuantum electrodynamicssymbols
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Renormalization group invariant matrix elements of Delta S = 2 and Delta I = 3/2 four fermion operators without quark masses

1999

We introduce a new parameterization of four-fermion operator matrix elements which does not involve quark masses and thus allows a reduction of systematic uncertainties. In order to simplify the matching between lattice and continuum renormalization schemes, we express our results in terms of renormalization group invariant B-parameters which are renormalization-scheme and scale independent. As an application of our proposal, matrix elements of DI=3/2 and SUSY DS =2 operators have been computed. The calculations have been performed using the tree-level improved Clover lattice action at two different values of the strong coupling constant (beta=6/g^2=6.0 and 6.2), in the quenched approximati…

QuarkNuclear and High Energy PhysicsHigh Energy Physics::LatticeSTANDARD MODELFOS: Physical sciencesWILSON FERMIONSQuenched approximationPartícules (Física nuclear)kaon decays gauge theory latticeLATTICE QCDRenormalizationHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeKAON B-PARAMETERLattice (order)Mathematical physicsPhysicsHigh Energy Physics - Lattice (hep-lat)FísicaFermionSupersymmetryInvariant (physics)Renormalization groupFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - PhenomenologyHigh Energy Physics::Experiment
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Heavy quark diffusion in an overoccupied gluon plasma

2020

We extract the heavy-quark diffusion coefficient \kappa and the resulting momentum broadening in a far-from-equilibrium non-Abelian plasma. We find several features in the time dependence of the momentum broadening: a short initial rapid growth of , followed by linear growth with time due to Langevin-type dynamics and damped oscillations around this growth at the plasmon frequency. We show that these novel oscillations are not easily explained using perturbative techniques but result from an excess of gluons at low momenta. These oscillation are therefore a gauge invariant confirmation of the infrared enhancement we had previously observed in gauge-fixed correlation functions. We argue that…

QuarkNuclear and High Energy PhysicsNuclear Theorynucl-thhep-latFOS: Physical sciencesLattice QCDhiukkasfysiikka01 natural sciences114 Physical sciencesNuclear Theory (nucl-th)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)fysikk0103 physical sciencesHeavy Quark Physicslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsPlasmonParticle Physics - PhenomenologyPhysics:Matematikk og Naturvitenskap: 400::Fysikk: 430 [VDP]010308 nuclear & particles physicsOscillationComputer Science::Information RetrievalHigh Energy Physics - Lattice (hep-lat)Particle Physics - Latticehep-phLattice QCDPlasmaInvariant (physics)GluonHigh Energy Physics - PhenomenologyQuantum electrodynamicsNuclear Physics - TheoryQuark–gluon plasmaQuark-Gluon Plasmalcsh:QC770-798
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NNLO Unquenched Calculation of the b Quark Mass

2000

By combining the first unquenched lattice computation of the B-meson binding energy and the two-loop contribution to the lattice HQET residual mass, we determine the (\bar{{MS}}) (b)-quark mass, (\bar{m}_{b}(\bar{m}_{b})). The inclusion of the two-loop corrections is essential to extract (\bar{m}_{b}(\bar{m}_{b})) with a precision of ({\cal O}(\Lambda^{2}_{QCD}/m_{b})), which is the uncertainty due to the renormalon singularities in the perturbative series of the residual mass. Our best estimate is (\bar{m}_{b}(\bar{m}_{b}) = (4.26 \pm 0.09) {\rm GeV}), where we have combined the different errors in quadrature. A detailed discussion of the systematic errors contributing to the final number …

QuarkNuclear and High Energy PhysicsParticle physicsB physics gauge theory latticeComputationB physics QCD latticeHigh Energy Physics::LatticeBinding energyLattice field theoryFOS: Physical sciencesElementary particleBottom quarkPartícules (Física nuclear)RenormalonHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Lattice (order)BibliographyPhysicsQuantum chromodynamicsHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)PropagatorFermionAtomic and Molecular Physics and OpticsFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - PhenomenologyStrange matterHigh Energy Physics::Experiment
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Light hadrons from lattice QCD with light (u, d), strange and charm dynamical quarks

2010

We present results of lattice QCD simulations with mass-degenerate up and down and mass-split strange and charm (N_f = 2+1+1) dynamical quarks using Wilson twisted mass fermions at maximal twist. The tuning of the strange and charm quark masses is performed at two values of the lattice spacing a~0.078 fm and a~0.086 fm with lattice sizes ranging from L~1.9 fm to L~2.8 fm. We measure with high statistical precision the light pseudoscalar mass m_PS and decay constant f_PS in a range 270 < m_PS < 510 MeV and determine the low energy parameters f_0, l_3 and l_4 of SU(2) chiral perturbation theory. We use the two values of the lattice spacing, several lattice sizes as well as different values of…

QuarkNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeHadronCharm quarkFOS: Physical sciencesLattice QCD2 FLAVORS01 natural sciencesCHIRAL PERTURBATION-THEORYCharm quarkLattice constantHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeTWISTED MASS FERMIONSChiral perturbation theoryWILSON QUARKS0103 physical sciencesddc:530ALGORITHM010306 general physicsSCALEPhysics010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaFermionLattice QCDSIMULATIONSPseudoscalarHigh Energy Physics - PhenomenologyLattice gauge theoryChiral LagrangiansYANG-MILLS THEORYHigh Energy Physics::ExperimentPHASE-STRUCTUREMESONChiral lagrangiansLight hadronsJournal of High Energy Physics
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Dynamical twisted mass fermions with light quarks

2007

We present results of dynamical simulations with 2 flavours of degenerate Wilson twisted mass quarks at maximal twist in the range of pseudo scalar masses from 300 to 550 MeV. The simulations are performed at one value of the lattice spacing a \lesssim 0.1 fm. In order to have O(a) improvement and aiming at small residual cutoff effects, the theory is tuned to maximal twist by requiring the vanishing of the untwisted quark mass. Precise results for the pseudo scalar decay constant and the pseudo scalar mass are confronted with chiral perturbation theory predictions and the low energy constants F, \bar{l}_3 and \bar{l}_4 are evaluated with small statistical errors.

QuarkNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryMONTE-CARLO ALGORITHMCHIRAL PERTURBATION-THEORY; MONTE-CARLO ALGORITHM; GROSS-NEVEU MODEL; YANG-MILLS THEORY; LATTICE QCD; PHASE-STRUCTURE; WILSON QUARKS; HMC ALGORITHM; GAUGE ACTIONS; 2 FLAVORSHigh Energy Physics::LatticeLattice field theoryScalar (mathematics)FOS: Physical sciences2 FLAVORSGAUGE ACTIONS01 natural sciences7. Clean energyCHIRAL PERTURBATION-THEORYLATTICE QCDHigh Energy Physics - LatticeGross–Neveu modelWILSON QUARKS0103 physical sciencesddc:530Twist010306 general physicsPhysics010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaGROSS-NEVEU MODELFermionLattice QCDSettore FIS/02 - Fisica Teorica Modelli e Metodi MatematiciYANG-MILLS THEORYPHASE-STRUCTUREHMC ALGORITHM
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Light meson physics from maximally twisted mass lattice QCD

2009

40 pages, 5 figures, 8 tables, 3 appendix.-- PACS: 11.15.Ha; 12.38.Gc; 12.39.Fe

QuarkNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryMesonHigh Energy Physics::LatticeFOS: Physical sciencesLattice QCD7. Clean energy01 natural sciencessymbols.namesakeHigh Energy Physics - LatticeLattice constantChiral perturbation theoryLattice (order)0103 physical sciences010306 general physicsPhysics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyLight mesonsMeson physicsFísicaFermionLattice QCDTwisted mass quarksQCDStrong interactions3. Good healthSettore FIS/02 - Fisica Teorica Modelli e Metodi MatematiciLattice QCD; Strong interactions; Meson physics; Twisted mass quarkssymbolsLow energy constantsLagrangian
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Effective Theories for QCD-like at TeV Scale

2014

We study the Effective Field Theory of three QCD-like theories, which can be classified by having quarks in a complex, real or pseudo-real representations of the gauge group. The Lagrangians are written in a very similar way so that the calculations can be done using techniques from Chiral Perturbation Theory (ChPT). We calculated the vacuum-expectation-value, the mass and the decay constant of pseudo-Goldstone Bosons up to next-to-next-to leading order (NNLO) \cite{Bijnens:2009qm}. The various channels of general $n$ flavour meson-meson scattering of the three theories are systematically studied and calculated up to NNLO \cite{Bijnens:2011fm}. We also calculated the vector, axial-vector, s…

QuarkNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryTechnicolorHigh Energy Physics::LatticeSpontaneous symmetry breakingNuclear TheoryFOS: Physical sciencesTechnicolorChiral Lagrangian01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeGauge group0103 physical sciencesEffective field theory010306 general physicsLattice Gauge Field TheoriesBosonPhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::Phenomenologychiral extrapolationSpontaneous Symmetry BreakingHigh Energy Physics - PhenomenologyComposite ModelsHigh Energy Physics::ExperimentNuclear and Particle Physics Proceedings
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Deep inelastic scattering on the quark-gluon plasma

2020

We provide an interpretation of the structure functions of a thermal medium such as the quark-gluon plasma in terms of the scattering of an incoming electron on the medium via the exchange of a spacelike photon. We then focus on the deep-inelastic scattering (DIS) regime, and formulate the corresponding moment sum rules obeyed by the structure functions. Accordingly, these moments are given by the thermal expectation value of twist-two operators, which is computable from first principles in lattice QCD for the first few moments. We also show how lattice QCD calculations can be used to probe how large the photon virtuality needs to be in order for the Bjorken scaling of structure functions t…

QuarkNuclear and High Energy PhysicsParticle physicsFOS: Physical scienceshep-latPartonLattice QCDExpectation value01 natural sciencesHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesPerturbative QCDlcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsParticle Physics - PhenomenologyPhysics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyPerturbative QCDParticle Physics - Latticehep-phLattice QCDRest frameDeep inelastic scatteringHigh Energy Physics - PhenomenologyQuark–gluon plasmaQuark-Gluon Plasmalcsh:QC770-798High Energy Physics::Experiment
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Dirac and Pauli form factors from lattice QCD

2011

We present a comprehensive analysis of the electromagnetic form factors of the nucleon from a lattice simulation with two flavors of dynamical O(a)-improved Wilson fermions. A key feature of our calculation is that we make use of an extensive ensemble of lattice gauge field configurations with four different lattice spacings, multiple volumes, and pion masses down to m_\pi ~ 180 MeV. We find that by employing Kelly-inspired parametrizations for the Q^2-dependence of the form factors, we are able to obtain stable fits over our complete ensemble. Dirac and Pauli radii and the anomalous magnetic moments of the nucleon are extracted and results at light quark masses provide evidence for chiral …

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeLattice field theoryNuclear TheoryFOS: Physical sciences7. Clean energy01 natural sciencessymbols.namesakePauli exclusion principleHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesddc:530Quantum field theory010306 general physicsQuantum chromodynamicsPhysics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)FermionLattice QCDJHigh Energy Physics - PhenomenologysymbolsNucleon
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