Search results for "lattice [space-time]"

showing 10 items of 692 documents

BK from the lattice with Wilson quarks

2004

We report our results for the bag-parameter BK obtained from the quenched simulations on the lattice with Wilson fermions at three values of the lattice spacing. We implemented the method by which no subtraction of the mixing with other four-fermion dS=2 operators is needed. Our final result, in terms of the renormalisation group invariant bag-parameter, is BK = 0.96 +/- 0.10.

QuarkPhysicsPhysics and Astronomy (miscellaneous)010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)FísicaFOS: Physical sciences[PHYS.HLAT] Physics [physics]/High Energy Physics - Lattice [hep-lat]Fermion01 natural sciencesHigh Energy Physics - LatticeLattice constantLattice (order)0103 physical sciences010306 general physicsEngineering (miscellaneous)Mathematical physics
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Inverse magnetic catalysis in nonlocal chiral quark models

2018

We study the behavior of strongly interacting matter under an external magnetic field in the context of nonlocal Polyakov-Nambu-Jona-Lasinio (PNJL) -like models. We find that at zero temperature the condensates display the well-known Magnetic Catalysis effect, showing a good quantitative agreement with lattice QCD results. Moreover, when extended to finite temperature we find that the Inverse Magnetic Catalysis effect is naturally incorporated.

QuarkPhysicsPolyakov-Nambu-Jona-Lasinio modelsHistoryCondensed matter physicsMagnetic catalysisHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyLattice field theoryCondensationFísicaInverseContext (language use)Lattice QCDComputer Science ApplicationsEducationMagnetic fieldQuarkMagnetic CatalysisCiencias ExactasJournal of Physics: Conference Series
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Nonperturbative renormalization and O(a) -improvement of the nonsinglet vector current with Nf=2+1 Wilson fermions and tree-level Symanzik improved g…

2019

In calculating hadronic contributions to precision observables for tests of the Standard Model in lattice QCD, the electromagnetic current plays a central role. Using a Wilson action with $\mathrm{O}(a)$ improvement in QCD with ${N}_{\mathrm{f}}$ flavors, a counterterm must be added to the vector current in order for its on-shell matrix elements to be $\mathrm{O}(a)$ improved. In addition, the local vector current, which has support on one lattice site, must be renormalized. At $\mathrm{O}(a)$, the breaking of the $\mathrm{SU}({N}_{\mathrm{f}})$ symmetry by the quark mass matrix leads to a mixing between the local currents of different quark flavors. We present a nonperturbative calculation…

QuarkPhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyLattice field theoryLattice QCDFermionMass matrix01 natural sciencesRenormalizationLattice (order)0103 physical sciences010306 general physicsMathematical physicsPhysical Review D
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Quark Contraction Tool -- QCT

2016

We present a Mathematica package for the calculation of Wick contractions in quantum field theories - QCT. Furthermore the package aims at automatically generating code for the calculation of physical matrix elements, suitable for numerical evaluation in a C++ program. To that end commonly used algebraic manipulations for the calculation of matrix elements in lattice QCD are implemented.

QuarkPhysicsQuantum chromodynamicsHigh Energy Physics - Lattice (hep-lat)Lattice field theoryFOS: Physical sciencesGeneral Physics and AstronomyLattice QCDDirected graphComputational Physics (physics.comp-ph)Symbolic computation01 natural sciences010305 fluids & plasmasAlgebraHigh Energy Physics - LatticeHardware and ArchitectureQuantum mechanics0103 physical sciencesComputer Science::Mathematical SoftwareAlgebraic numberQuantum field theory010306 general physicsPhysics - Computational Physics
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Probing the chiral weak Hamiltonian at finite volumes

2006

Non-leptonic kaon decays are often described through an effective chiral weak Hamiltonian, whose couplings ("low-energy constants") encode all non-perturbative QCD physics. It has recently been suggested that these low-energy constants could be determined at finite volumes by matching the non-perturbatively measured three-point correlation functions between the weak Hamiltonian and two left-handed flavour currents, to analytic predictions following from chiral perturbation theory. Here we complete the analytic side in two respects: by inspecting how small ("epsilon-regime") and intermediate or large ("p-regime") quark masses connect to each other, and by including in the discussion the two …

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsChiral perturbation theoryHigh Energy Physics - Lattice (hep-lat)FlavourHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaObservableweak decaysPseudoscalarsymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Latticelattice QCDkaon physicssymbolschiral lagrangiansHamiltonian (quantum mechanics)Mathematical physics
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Abelian dominance and the dual Meissner effect in local unitary gauges in SU(2) gluodynamics

2007

Performing highly precise Monte-Carlo simulations of SU(2) gluodynamics, we observe for the first time Abelian dominance in the confining part of the static potential in local unitary gauges such as the F12 gauge. We also study the flux-tube profile between the quark and antiquark in these local unitary gauges and find a clear signal of the dual Meissner effect. The Abelian electric field is found to be squeezed into a flux tube by the monopole supercurrent. This feature is the same as that observed in the non-local maximally Abelian gauge. These results suggest that the Abelian confinement scenario is gauge independent. Observing the important role of space-like monopoles in the Polyakov g…

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeLattice field theoryHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)Magnetic monopoleFOS: Physical sciencesGluonHigh Energy Physics::TheoryHigh Energy Physics - LatticeMeissner effectQuantum electrodynamicsAbelian groupSpecial unitary groupMathematical physics
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Δ-baryon electromagnetic form factors in lattice QCD

2008

We develop techniques to calculate the four Delta electromagnetic form factors using lattice QCD, with particular emphasis on the sub-dominant electric quadrupole form factor that probes deformation of the Delta. Results are presented for pion masses down to approximately 350 MeV for three cases: quenched QCD, two flavors of dynamical Wilson quarks, and three flavors of quarks described by a mixed action combining domain wall valence quarks and dynamical staggered sea quarks. The magnetic moment of the Delta is chirally extrapolated to the physical point and the Delta charge density distributions are discussed.

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeLattice field theoryHigh Energy Physics - Lattice (hep-lat)Nuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesLattice QCDDelta baryonBaryonHigh Energy Physics - LatticePionLattice gauge theoryHigh Energy Physics::Experiment
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Flavour symmetry restoration and kaon weak matrix elements in quenched twisted mass QCD

2007

We simulate two variants of quenched twisted mass QCD (tmQCD), with degenerate Wilson quarks of masses equal to or heavier than half the strange quark mass. We use Ward identities in order to measure the twist angles of the theory and thus check the quality of the tuning of mass parameters to a physics condition which stays constant as the lattice spacing is varied. Flavour symmetry breaking in tmQCD is studied in a framework of two fully twisted and two standard Wilson quark flavours, tuned to be degenerate in the continuum. Comparing pseudoscalar masses, obtained from connected quark diagrams made of tmQCD and/or standard Wilson quark propagators, we confirm that flavour symmetry breaking…

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsStrange quarkHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Degenerate energy levelsLattice field theoryFlavourHigh Energy Physics::PhenomenologyFOS: Physical sciencesParticle Physics - LatticePseudoscalarHigh Energy Physics - LatticeHigh Energy Physics::ExperimentSymmetry breaking
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Test of the heavy quark-light diquark approximation for baryons with a heavy quark

2008

We check a commonly used approximation in which a baryon with a heavy quark is described as a heavy quark-light diquark system. The heavy quark influences the diquark internal motion reducing the average distance between the two light quarks. Besides, we show how the average distance between the heavy quark and any of the light quarks, and that between the heavy quark and the center of mass of the light diquark, are smaller than the distance between the two light quarks, which seems to contradict the heavy quark-light diquark picture. This latter result is in agreement with expectations from QCD sum rules and lattice QCD calculations. Our results also show that the diquark approximations pr…

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsQCD sum rulesParticle physicsNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaLattice QCDNuclear Theory (nucl-th)DiquarkNuclear physicsBaryonCharmed baryonsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentCenter of massNuclear Experiment
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Up, down, strange and charm quark masses withNf=2+1+1twisted mass lattice QCD

2014

Abstract We present a lattice QCD calculation of the up, down, strange and charm quark masses performed using the gauge configurations produced by the European Twisted Mass Collaboration with N f = 2 + 1 + 1 dynamical quarks, which include in the sea, besides two light mass degenerate quarks, also the strange and charm quarks with masses close to their physical values. The simulations are based on a unitary setup for the two light quarks and on a mixed action approach for the strange and charm quarks. The analysis uses data at three values of the lattice spacing and pion masses in the range 210 – 450 MeV , allowing for accurate continuum limit and controlled chiral extrapolation. The quark …

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsStrange quarkParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryLattice QCD7. Clean energySigma baryonCharm quarkNuclear physicsPionUp quarkHigh Energy Physics::ExperimentNuclear ExperimentNuclear Physics B
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