Search results for "lattice [space-time]"

showing 10 items of 692 documents

Nucleon mass and pion-nucleon sigma term from a chiral analysis of lattice QCD data

2013

The pion mass dependence of the nucleon mass within the covariant SU(2) baryon chiral perturbation theory both without and with explicit Delta(1232) degrees of freedom up to order p(4) is investigated. By fitting to a comprehensive set of lattice QCD data in 2 and 2 + 1 flavors from several collaborations, for pion masses M-pi < 420 MeV, we obtain low energy constants of natural size that are compatible with pion-nucleon scattering data. Our results are consistent with the rather linear pion mass dependence showed by lattice QCD. In the 2 flavor case we have also performed simultaneous fits to nucleon mass and sigma(pi N) data. As a result of our analysis, which encompasses the study of fin…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theory010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryOrder (ring theory)Light hadron massesLattice QCD01 natural sciencesResonance (particle physics)Perturbation-theoryBaryonPion0103 physical sciencesHigh Energy Physics::ExperimentFísica nuclearPerturbation theory010306 general physicsNucleonNuclear Experiment
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The scalar pion form factor in two-flavor lattice QCD

2013

We calculate the scalar form factor of the pion using two dynamical flavors of non-perturbatively $\mathcal{O}(a)$-improved Wilson fermions, including both the connected and the disconnected contribution to the relevant correlation functions. We employ the calculation of all-to-all propagators using stochastic sources and a generalized hopping parameter expansion. From the form factor data at vanishing momentum transfer, $Q^2=0$, and two non-vanishing $Q^2$ we obtain an estimate for the scalar radius $\left^\pi_{_{\rm S}}$ of the pion at one value of the lattice spacing and for five different pion masses. Using Chiral Perturbation Theory at next-to-leading order, we find $\left^\pi_{_{\rm S…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Momentum transferScalar (mathematics)Form factor (quantum field theory)FOS: Physical sciencesOrder (ring theory)PropagatorLattice QCDHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PionHigh Energy Physics - Lattice
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Charm mass dependence of the weak Hamiltonian in chiral perturbation theory

2004

Suppose that the weak interaction Hamiltonian of four-flavour SU(4) chiral effective theory is known, for a small charm quark mass m_c. We study how the weak Hamiltonian changes as the charm quark mass increases, by integrating it out within chiral perturbation theory to obtain a three-flavour SU(3) chiral theory. We find that the ratio of the SU(3) low-energy constants which mediate Delta I=1/2 and Delta I=3/2 transitions, increases rather rapidly with m_c, as \sim m_c ln (1/m_c). The logarithmic effect originates from "penguin-type" charm loops, and could represent one of the reasons for the Delta I=1/2 rule.

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryLogarithmHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesWeak interactionweak decaysCharm quarksymbols.namesakeHigh Energy Physics - Phenomenologylattice QCDHigh Energy Physics - Phenomenology (hep-ph)kaon physicssymbolsEffective field theorychiral lagrangiansHigh Energy Physics::ExperimentHamiltonian (quantum mechanics)
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Non-perturbative improvement of the vector current in Wilson lattice QCD

2015

Many observables of interest in lattice QCD are extracted from correlation functions involving the vector current. If Wilson fermions are used, it is therefore of practical importance that, besides the action, the current be O($a$) improved in order to remove the leading discretization errors from the observables. Here we introduce and apply a new method to determine the improvement coefficient for the two most widely used discretizations of the current.

PhysicsNuclear and High Energy PhysicsParticle physicsCurrent (mathematics)DiscretizationHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Order (ring theory)FOS: Physical sciencesObservableLattice QCDFermionAction (physics)Theoretical physicsHigh Energy Physics - LatticeLattice gauge theory
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S-waveKK*interactions in a finite volume and thef1(1285)

2015

Lattice QCD simulations provide a promising way to disentangle different interpretations of hadronic resonances, which might be of particular relevance to understand the nature of the so-called XY Z particles. Recent studies have shown that in addition to the well-established naive quark model picture, the axial-vector meson f1(1285) can also be understood as a dynamically generated state built upon the KK ∗ interaction. In this work, we calculate the energy levels of the KK ∗ system in the f1(1285) channel in finite volume using the chiral unitary approach. We propose to calculate the loop function in the dimensional regularization scheme, which is equivalent to the hybrid approach adopted…

PhysicsNuclear and High Energy PhysicsParticle physicsFinite volume methodMesonUnitarity010308 nuclear & particles physicsHigh Energy Physics::LatticeQuark modelLattice field theoryLattice QCD01 natural sciencesDimensional regularization0103 physical sciencesBound state010306 general physicsMathematical physicsPhysical Review D
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Finite volume treatment of ππ scattering and limits to phase shifts extraction from lattice QCD

2012

We study theoretically the effects of finite volume for pipi scattering in order to extract physical observables for infinite volume from lattice QCD. We compare three different approaches for pipi scattering (lowest order Bethe-Salpeter approach, N/D and inverse amplitude methods) with the aim to study the effects of the finite size of the box in the potential of the different theories, specially the left-hand cut contribution through loops in the crossed t,u-channels. We quantify the error made by neglecting these effects in usual extractions of physical observables from lattice QCD spectra. We conclude that for pipi phase-shifts in the scalar-isoscalar channel up to 800 MeV this effect i…

PhysicsNuclear and High Energy PhysicsParticle physicsFinite volume methodScatteringHigh Energy Physics - Lattice (hep-lat)Phase (waves)FOS: Physical sciencesFísicaInverseObservableLattice QCDHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeAmplitudeIsospinJournal of High Energy Physics
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Running soft parameters in SUSY models with multiple U(1) gauge factors

2012

Abstract We generalize the two-loop renormalization group equations for the parameters of the softly broken SUSY gauge theories given in the literature to the most general case when the gauge group contains more than a single Abelian gauge factor. The complete method is illustrated at two-loop within a specific example and compared to some of the previously proposed partial treatments.

PhysicsNuclear and High Energy PhysicsParticle physicsIntroduction to gauge theoryQuantum gauge theory010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::Phenomenology01 natural sciencesBRST quantizationHigh Energy Physics::TheoryTheoretical physicsHamiltonian lattice gauge theorySupersymmetric gauge theoryLattice gauge theory0103 physical sciences010306 general physicsGauge anomalyGauge fixingNuclear Physics B
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Chiral corrections to the 1 −+ exotic meson mass

2016

We first construct the effective chiral Lagrangians for the $1^{-+}$ exotic mesons. With the infrared regularization scheme, we derive the one-loop infrared singular chiral corrections to the $\pi_1(1600)$ mass explicitly. We investigate the variation of the different chiral corrections with the pion mass under two schemes. Hopefully, the explicit non-analytical chiral structures will be helpful to the chiral extrapolation of the lattice data from the dynamical lattice QCD simulation of either the exotic light hybrid meson or tetraquark state.

PhysicsNuclear and High Energy PhysicsParticle physicsMeson010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyExtrapolationFOS: Physical sciencesAstronomy and AstrophysicsLattice QCD01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticePionLattice (order)Regularization (physics)0103 physical sciencesTetraquarkExotic meson010306 general physicsInstrumentationChinese Physics C
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Improved $K_{e3}$ radiative corrections sharpen the $K_{\mu 2}$--$K_{l3}$ discrepancy

2021

The measurements of $V_{us}$ in leptonic $(K_{\mu 2})$ and semileptonic $(K_{l3})$ kaon decays exhibit a $3\sigma$ disagreement, which could originate either from physics beyond the Standard Model or some large unidentified Standard Model systematic effects. Clarifying this issue requires a careful examination of all existing Standard Model inputs. Making use of a newly-proposed computational framework and the most recent lattice QCD results, we perform a comprehensive re-analysis of the electroweak radiative corrections to the $K_{e3}$ decay rates that achieves an unprecedented level of precision of $10^{-4}$, which improves the current best results by almost an order of magnitude. No larg…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theory010308 nuclear & particles physicsPhysics beyond the Standard ModelElectroweak interactionLattice QCDLattice QCDQC770-79801 natural sciencesStandard ModelHigh Energy Physics - ExperimentKaon PhysicsHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeNuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesRadiative transferPrecision QEDHigh Energy Physics::Experiment010306 general physicsNuclear ExperimentOrder of magnitude
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Spin-dependent potentials from lattice QCD

2006

The spin-dependent corrections to the static inter-quark potential are phenomenologically relevant to describing the fine and hyperfine spin splitting of the heavy quarkonium spectra. We investigate these corrections, which are represented as the field strength correlators on the quark-antiquark source, in SU(3) lattice gauge theory. We use the Polyakov loop correlation function as the quark-antiquark source, and by employing the multi-level algorithm, we obtain remarkably clean signals for these corrections up to intermediate distances of around 0.6 fm. Our observation suggests several new features of the corrections.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::LatticeLattice field theoryHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesField strengthLattice QCDQuarkoniumNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - LatticeHamiltonian lattice gauge theoryHigh Energy Physics - Phenomenology (hep-ph)Lattice gauge theoryQuantum electrodynamicsHyperfine structureLattice model (physics)
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