Search results for "High Energy Physics - Lattice"

showing 10 items of 466 documents

Nonperturbative renormalization in coordinate space

2003

We present an exploratory study of a gauge-invariant non-perturbative renormalization technique. The renormalization conditions are imposed on correlation functions of composite operators in coordinate space on the lattice. Numerical results for bilinears obtained with overlap and O(a)-improved Wilson fermions are presented. The measurement of the quark condensate is also discussed.

QuarkPhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)field theory gauge theory lattice renormalizationFOS: Physical sciencesFísicaParticle Physics - LatticeFermionAtomic and Molecular Physics and OpticsComposite operatorRenormalizationFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - LatticeLattice (order)Non-perturbativeCoordinate spaceMathematical physics
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Nucleon matrix elements from lattice QCD with all-mode-averaging and a domain-decomposed solver: An exploratory study

2017

We study the performance of all-mode-averaging (AMA) when used in conjunction with a locally deflated SAP-preconditioned solver, determining how to optimize the local block sizes and number of deflation fields in order to minimize the computational cost for a given level of overall statistical accuracy. We find that AMA enables a reduction of the statistical error on nucleon charges by a factor of around two at the same cost when compared to the standard method. As a demonstration, we compute the axial, scalar and tensor charges of the nucleon in $N_f=2$ lattice QCD with non-perturbatively O(a)-improved Wilson quarks, using O(10,000) measurements to pursue the signal out to source-sink sepa…

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Scalar (physics)FOS: Physical sciencesCharge (physics)Lattice QCDComputational Physics (physics.comp-ph)Solver01 natural sciencesMatrix (mathematics)High Energy Physics - Lattice13. Climate actionQuantum electrodynamics0103 physical scienceslcsh:QC770-798ddc:530lcsh:Nuclear and particle physics. Atomic energy. RadioactivityTensor010306 general physicsNucleonPhysics - Computational PhysicsNuclear Physics B
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Lattice-constrained parametrizations of form factors for semileptonic and rare radiative B decays

1997

We describe the form factors for B to rho lepton neutrino and B to K* gamma decays with just two parameters and the two form factors for B to pi lepton neutrino with a further two or three parameters. The parametrizations are consistent with heavy quark symmetry, kinematic constraints and lattice results, which we use to determine the parameters. In addition, we test versions of the parametrizations consistent (or not) with light-cone sum rule scaling relations at q^2=0.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::Phenomenologyhep-latLattice QCD calculationFOS: Physical sciencesFísicaAtomic and Molecular Physics and OpticsSemileptonic and rare radiative decays of B mesonsHigh Energy Physics - LatticeDetermination of Cabibbo-Kobayashi-Maskawa matrix elementsLattice (order)Radiative transferHigh Energy Physics::ExperimentSum rule in quantum mechanicsNeutrinoScalingHeavy quark effective theoryTwo-formLepton
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Lattice quark masses: a non-perturbative measurement

1998

We discuss the renormalization of different definitions of quark masses in the Wilson and the tree-level improved SW-Clover fermionic action. For the improved case we give the correct relationship between the quark mass and the hopping parameter. Using perturbative and non-perturbative renormalization constants, we extract quark masses in the $\MSbar$ scheme from Lattice QCD in the quenched approximation at $\beta=6.0$, $\beta=6.2$ and $\beta=6.4$ for both actions. We find: $\bar{m}^{\MSbar}(2 GeV)=5.7 \pm 0.1 \pm 0.8$ MeV, $m_s^{\MSbar}(2GeV)= 130 \pm 2 \pm 18 $ MeV and $m_c^{\MSbar}(2 GeV) = 1662\pm 30\pm 230$ MeV.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyLattice (group)FOS: Physical sciencesFísicaQuenched approximationLattice QCDRenormalizationFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeQCD quark masses latticeBeta (velocity)High Energy Physics::ExperimentNon-perturbativeNuclear ExperimentBar (unit)
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Non-perturbative renormalisation of left left four-fermion operators with Neuberger fermions

2006

We outline a general strategy for the non-perturbative renormalisation of composite operators in discretisations based on Neuberger fermions, via a matching to results obtained with Wilson-type fermions. As an application, we consider the renormalisation of the four-quark operators entering the Delta S=1 and Delta S=2 effective Hamiltonians. Our results are an essential ingredient for the determination of the low-energy constants governing non-leptonic kaon decays.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)field theory gauge theory lattice renormalizationHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaParticle Physics - LatticeFermionComposite operatorRenormalizationFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - LatticeOperator (computer programming)High Energy Physics::ExperimentNon-perturbativeMathematical physics
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Heavy Baryon Specroscopy from the Lattice

1996

The results of an exploratory lattice study of heavy baryon spectroscopy are presented. We have computed the full spectrum of the eight baryons containing a single heavy quark, on a $24^3\times 48$ lattice at $\beta=6.2$, using an $O(a)$-improved fermion action. We discuss the lattice baryon operators and give a method for isolating the contributions of the spin doublets $(\Sigma,\Sigma^*)$, $(\Xi',\Xi^*)$ and $(\Omega,\Omega^*)$ to the correlation function of the relevant operator. We compare our results with the available experimental data and find good agreement in both the charm and the beauty sectors, despite the long extrapolation in the heavy quark mass needed in the latter case. We …

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeLattice field theoryNuclear TheoryHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)FísicaFOS: Physical sciencesFermionOmegaNuclear physicsBaryonCharmed baryonsHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Lattice (order)High Energy Physics::ExperimentNuclear Experiment
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First lattice calculation of the B-meson binding and kinetic energies

1995

We present the first lattice calculation of the B-meson binding energy $\labar$ and of the kinetic energy $-\lambda_1/2 m_Q$ of the heavy-quark inside the pseudoscalar B-meson. This calculation has required the non-perturbative subtraction of the power divergences present in matrix elements of the Lagrangian operator $\bar h D_4 h$ and of the kinetic energy operator $\bar h \vec D^2 h$. The non-perturbative renormalisation of the relevant operators has been implemented by imposing suitable renormalisation conditions on quark matrix elements, in the Landau gauge. Our numerical results have been obtained from several independent numerical simulations at $\beta=6.0$ and $6.2$, and using, for t…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyBinding energyFOS: Physical sciencesFísicaKinetic energyLambdaUpper and lower boundsPseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentB mesonParticle Physics - Phenomenology
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Geometrical volume effects in the computation of the slope of the isgur-wise function

1994

We use a method recently suggested for evaluating the slope of the Isgur-Wise function, at the zero-recoil point, on the lattice. The computations are performed in the quenched approximation to lattice QCD, on a $24^3 \times 48$ lattice at $\beta=6.2$, using an $O(a)$-improved action for the fermions. We have found unexpectedly large finite-volume effects in such a calculation. These volume corrections turned out to be purely geometrical and independent of the dynamics of the system. After the study of these effects on a smaller volume and for different quark masses, we give approximate expressions that account for them. Using these approximations we find $\xi^\prime(1)=-1.7 \pm 0.2$ and $\…

QuarkPhysicsNuclear and High Energy PhysicsStrange quarkParticle physicsMesonHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyDown quarkFOS: Physical sciencesFísicaQuenched approximationLattice QCDCharm quarkHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Up quarkHigh Energy Physics::Experiment
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Nonperturbative renormalization of quark bilinears

1998

We compute non-perturbatively the renormalization constants of quark bilinears on the lattice in the quenched approximation at three values of the coupling beta=6/g_0^2=6.0,6.2,6.4 using both the Wilson and the tree-level improved SW-Clover fermion action. We perform a Renormalization Group analysis at the next-to-next-to-leading order and compute Renormalization Group invariant values for the constants. The results are applied to obtain a fully non-perturbative estimate of the vector and pseudoscalar decay constants.

QuarkPhysicsNuclear and High Energy Physicsgauge theory lattice non-perturbative renormalizationHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)FísicaFOS: Physical sciencesQuenched approximationFermionRenormalization groupRenormalizationPseudoscalarFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - LatticeLattice (order)Non-perturbativeMathematical physics
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Splittings of low-lying charmonium masses at the physical point

2019

We present high-precision results from lattice QCD for the mass splittings of the low-lying charmonium states. For the valence charm quark, the calculation uses Wilson-clover quarks in the Fermilab interpretation. The gauge-field ensembles are generated in the presence of up, down, and strange sea quarks, based on the improved staggered (asqtad) action, and gluon fields, based on the one-loop, tadpole-improved gauge action. We use five lattice spacings and two values of the light sea quark mass to extrapolate the results to the physical point. An enlarged set of interpolating operators is used for a variational analysis to improve the determination of the energies of the ground states in ea…

QuarkPhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)ExtrapolationFOS: Physical sciencesLattice QCD01 natural sciencesCharm quarkGluonddc:High Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Lattice (order)0103 physical sciencesHigh Energy Physics::ExperimentFermilab010306 general physicsHyperfine structure
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