Search results for "lattice qcd"

showing 10 items of 241 documents

Direct calculation of hadronic light-by-light scattering

2015

We report calculations of hadronic light-by-light scattering amplitudes via lattice QCD evaluation of Euclidean four-point functions of vector currents. These initial results include only the fully quark-connected contribution. Particular attention is given to the case of forward scattering, which can be related via dispersion relations to the $\gamma^* \gamma^* \to$ hadrons cross section, and thus allows lattice data to be compared with phenomenology. We also present a strategy for computing the hadronic light-by-light contribution to the muon anomalous magnetic moment.

PhysicsQuantum chromodynamicsParticle physicsMuonAnomalous magnetic dipole momentNuclear TheoryLattice field theoryHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical sciencesLattice QCDLight scatteringScattering amplitudeNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeHigh Energy Physics::ExperimentPhenomenology (particle physics)
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Review of Lattice QCD Studies of Hadronic Vacuum Polarization Contribution to Muon g-2

2019

Lattice QCD (LQCD) studies for the hadron vacuum polarization (HVP) and its contribution to the muon anomalous magnetic moment (muon g-2) are reviewed. There currently exists more than 3-sigma deviations in the muon g-2 between the BNL experiment with 0.5 ppm precision and the Standard Model (SM) predictions, where the latter relies on the QCD dispersion relation for the HVP. The LQCD provides an independent crosscheck of the dispersive approaches and important indications for assessing the SM prediction with measurements at ongoing/forthcoming experiments at Fermilab/J-PARC (0.14/0.1 ppm precision). The LQCD has made significant progress, in particular, in the long distance and finite volu…

PhysicsQuantum chromodynamicsParticle physicsMuonAnomalous magnetic dipole momentPhysics beyond the Standard ModelHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesLattice QCDHigh Energy Physics - LatticeIsospinHigh Energy Physics::ExperimentFermilabVacuum polarization
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Strong magnetic fields in a nonlocal Polyakov chiral quark model

2018

We study the behavior of strongly interacting matter under an external constant magnetic field in the context of nonlocal chiral quark models that incorporate a coupling to the Polyakov loop. We find that at zero temperature the behavior of the quark condensates shows the expected magnetic catalysis effect, our predictions being in good quantitative agreement with lattice QCD results. On the other hand when the analysis is extended to the case of finite temperature our results show that nonlocal models naturally lead to the Inverse Magnetic Catalysis effect for both the chiral restoration and deconfinement transition temperatures.

PhysicsQuantum chromodynamicsQuarkCiencias Astronómicas010308 nuclear & particles physicsMagnetic catalysisPhysicsQC1-999High Energy Physics::LatticeHigh Energy Physics::PhenomenologyLattice field theoryQuark modelLattice QCD01 natural sciencesDeconfinementMagnetic fieldQuantum electrodynamics0103 physical sciencesNonlocal chiral quark models010306 general physicsCiencias ExactasQuantum chromodynamicsEPJ Web of Conferences
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Nucleon axial charge in lattice QCD with controlled errors

2012

We report on our calculation of the nucleon axial charge ${g}_{\mathrm{A}}$ in QCD with two flavors of dynamical quarks. A detailed investigation of systematic errors is performed, with a particular focus on contributions from excited states to three-point correlation functions. The use of summed operator insertions allows for a much better control over such contamination. After performing a chiral extrapolation to the physical pion mass, we find ${g}_{\mathrm{A}}=1.223\ifmmode\pm\else\textpm\fi{}0.063(\mathrm{stat}{)}_{\ensuremath{-}0.060}^{+0.035}(\mathrm{syst})$, in good agreement with the experimental value.

PhysicsQuantum chromodynamicsQuarkNuclear and High Energy PhysicsParticle physicsPionHigh Energy Physics::LatticeLattice field theoryHigh Energy Physics::ExperimentCharge (physics)Lattice QCDCorrelation function (quantum field theory)NucleonPhysical Review D
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Quark transverse charge densities in the from lattice QCD

2009

Abstract We extend the formalism relating electromagnetic form factors to transverse quark charge densities in the light-front frame to the case of a spin-3/2 baryon and calculate these transverse densities for the Δ ( 1232 ) isobar using lattice QCD. The transverse charge densities for a transversely polarized spin-3/2 particle are characterized by monopole, dipole, quadrupole, and octupole patterns representing the structure beyond that of a pure point-like spin-3/2 particle. We present lattice QCD results for the Δ-isobar electromagnetic form factors for pion masses down to approximatively 350 MeV for three cases: quenched QCD, two-degenerate flavors of dynamical Wilson quarks, and three…

PhysicsQuantum chromodynamicsQuarkNuclear and High Energy PhysicsParticle physicsPoint particleHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryLattice field theoryCharge densityLattice QCDBaryonPionQuantum electrodynamicsHigh Energy Physics::ExperimentNuclear ExperimentNuclear Physics A
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Measurement of theB¯0→D*+ℓ−ν¯ℓdecay rate and|Vcb|

2005

We present a measurement of the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cb}|$ based on a sample of about 53,700 \mbox{$\Bzb \rightarrow D^{*+} \ell^- \bar{\nu}_{\ell}$} decays observed by the \babar\ detector. We obtain the branching fraction averaged over $\ell = e,\mu$, ${\cal B}(\Bzb \rightarrow D^{*+} \ell^- \bar{\nu}_{\ell}) = (4.90 \pm 0.07\mathrm{(stat.)}^{+0.36}_{-0.35}\mathrm{(syst.)})\%$. We measure the differential decay rate as a function of $w$, the relativistic boost $\gamma$ of the $D^{*+}$ in the ${\Bzb}$ rest frame. By extrapolating $d\Gamma/dw$ to the kinematic limit $w \rightarrow 1$, we extract the product of $|V_{cb}|$ and the axial form factor ${\cal A}_1(w=1)$. …

PhysicsQuantum chromodynamicsSemileptonic decayNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyForm factor (quantum field theory)Lattice QCD01 natural sciencesParticle identificationClassical mechanicsProduct (mathematics)0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsBar (unit)Physical Review D
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Total decay and transition rates from LQCD

2018

We present a new technique for extracting total transition rates into final states with any number of hadrons from lattice QCD. The method involves constructing a finite-volume Euclidean four-point function whose corresponding infinite-volume spectral function gives access to the decay and transition rates into all allowed final states. The inverse problem of calculating the spectral function is solved via the Backus-Gilbert method, which automatically includes a smoothing procedure. This smoothing is in fact required so that an infinite-volume limit of the spectral function exists. Using a numerical toy example we find that reasonable precision can be achieved with realistic lattice data. …

PhysicsQuantum chromodynamicsToy model010308 nuclear & particles physicsPhysicsQC1-999Lattice field theoryLattice QCDInverse problemDeep inelastic scattering01 natural sciencesLattice (order)0103 physical sciencesStatistical physics010306 general physicsSmoothingEPJ Web of Conferences
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Non-Perturbative Propagators in QCD

1994

Over the last two decades it has become clear that perturbation theory can only give us very limited information about QCD. For example it is not sufficient to describe that most basic of things, the mass spectrum. Although, we may hope one day to gain from the lattice approach numerical confirmation that we have the correct Lagrangian to describe hadronic physics, that day is not at hand. In the meantime it will be argued here, the operator product expansion (OPE) offers us some useful non-perturbative information about the structure of QCD.

PhysicsQuantum chromodynamicssymbols.namesakeTheoretical physicsLattice (order)High Energy Physics::PhenomenologyHadronsymbolsPropagatorLattice QCDOperator product expansionNon-perturbativeLagrangian
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Non-perturbative renormalization of static-light four-fermion operators in quenched lattice QCD

2007

We perform a non-perturbative study of the scale-dependent renormalization factors of a multiplicatively renormalizable basis of $\Delta{B}=2$ parity-odd four-fermion operators in quenched lattice QCD. Heavy quarks are treated in the static approximation with various lattice discretizations of the static action. Light quarks are described by non-perturbatively ${\rm O}(a)$ improved Wilson-type fermions. The renormalization group running is computed for a family of Schroedinger functional (SF) schemes through finite volume techniques in the continuum limit. We compute non-perturbatively the relation between the renormalization group invariant operators and their counterparts renormalized in …

PhysicsQuarkNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Lattice field theoryFOS: Physical sciencesParticle Physics - LatticeLattice QCDFermionRenormalization groupRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeLattice (order)lattice gauge field theories; lattice qcd; lattice quantum field theoryNon-perturbativeMathematical physics
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The negative-parity spin-1/2 Λ baryon spectrum from lattice QCD and effective theory

2021

The spectrum of the negative-parity spin-1/2 $\Lambda$ baryons is studied using lattice QCD and hadronic effective theory in a unitarized coupled-channel framework. A direct comparison between the two approaches is possible by considering the hadronic effective theory in a finite volume and with hadron masses and mesonic decay constants that correspond to the situation studied on the lattice. Comparing the energy level spectrum and $SU(3)$ flavor decompositions of the individual states, it is found that the lowest two states extracted from lattice QCD can be identified with one of the two $\Lambda(1405)$-poles and the $\Lambda(1670)$ resonance. The quark mass dependences of these two lattic…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsFinite volume method010308 nuclear & particles physicsHigh Energy Physics::LatticePhysicsQC1-999HadronNuclear TheoryHigh Energy Physics::PhenomenologyParity (physics)Lattice QCD01 natural sciencesBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeLattice (order)0103 physical sciencesEffective field theoryHigh Energy Physics::Experiment010306 general physicsPhysics Letters B
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