Search results for "lattice qcd"

showing 10 items of 241 documents

Vacuum correlators at short distances from lattice QCD

2021

Non-perturbatively computing the hadronic vacuum polarization at large photon virtualities and making contact with perturbation theory enables a precision determination of the electromagnetic coupling at the $Z$ pole, which enters global electroweak fits. In order to achieve this goal ab initio using lattice QCD, one faces the challenge that, at the short distances which dominate the observable, discretization errors are hard to control. Here we address challenges of this type with the help of static screening correlators in the high-temperature phase of QCD, yet without incurring any bias. The idea is motivated by the observations that (a) the cost of high-temperature simulations is typica…

Nuclear and High Energy PhysicsHigh Energy Physics::Latticepolecostshep-latFOS: Physical sciencesLattice QCDQC770-798nonperturbativeoperator product expansion53001 natural sciences7. Clean energythermal [correlation function]lattice [perturbation theory]High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Nuclear and particle physics. Atomic energy. Radioactivityprecision measurement [electroweak interaction]quantum chromodynamics0103 physical sciencesPerturbative QCDhadronic [vacuum polarization]ddc:530010306 general physicsParticle Physics - Phenomenology010308 nuclear & particles physicsscreeningComputer Science::Information RetrievalphotonHigh Energy Physics - Lattice (hep-lat)lattice field theorytemperaturehep-phParticle Physics - LatticeHigh Energy Physics - Phenomenologyelectromagnetic [coupling]flavor [quark]Journal of High Energy Physics
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The subtraction contribution to the muonic-hydrogen Lamb shift: a point for lattice QCD calculations of the polarizability effect

2020

The proton-polarizability contribution to the muonic-hydrogen Lamb shift is a major source of theoretical uncertainty in the extraction of the proton charge radius. An empirical evaluation of this effect, based on the proton structure functions, requires a systematically improvable calculation of the "subtraction function", possibly using lattice QCD. We consider a different subtraction point, with the aim of accessing the subtraction function directly in lattice calculations. A useful feature of this subtraction point is that the corresponding contribution of the structure functions to the Lamb shift is suppressed. The whole effect is dominated by the subtraction contribution, calculable o…

Nuclear and High Energy PhysicsNuclear TheoryAtomic Physics (physics.atom-ph)FOS: Physical sciences01 natural sciencesPhysics - Atomic PhysicsNuclear Theory (nucl-th)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Charge radiusPolarizabilityLattice (order)0103 physical sciencesPhysics::Atomic Physics010306 general physicsExotic atomPhysics010308 nuclear & particles physicsStructure functionHigh Energy Physics - Lattice (hep-lat)SubtractionLattice QCD3. Good healthLamb shiftHigh Energy Physics - PhenomenologyQuantum electrodynamics
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Implementing the three-particle quantization condition including higher partial waves

2019

We present an implementation of the relativistic three-particle quantization condition including both $s$- and $d$-wave two-particle channels. For this, we develop a systematic expansion about threshold of the three-particle divergence-free K matrix, $\mathcal{K}_{\mathrm{df,3}}$, which is a generalization of the effective range expansion of the two-particle K matrix, $\mathcal{K}_2$. Relativistic invariance plays an important role in this expansion. We find that $d$-wave two-particle channels enter first at quadratic order. We explain how to implement the resulting multichannel quantization condition, and present several examples of its application. We derive the leading dependence of the …

Nuclear and High Energy PhysicsNuclear TheoryAtomic Physics (physics.atom-ph)Relativistic invarianceFOS: Physical sciencesLattice QCD01 natural sciencesPhysics - Atomic PhysicsNuclear Theory (nucl-th)Quantization (physics)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBound statelcsh:Nuclear and particle physics. Atomic energy. RadioactivityQuadratic orderScattering Amplitudes010306 general physicsNuclear theoryCondensed Matter - Statistical MechanicsK matrixMathematical physicsPhysicsLattice Quantum Field TheoryStatistical Mechanics (cond-mat.stat-mech)010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Lattice QCDScattering amplitudeHigh Energy Physics - Phenomenologylcsh:QC770-798Journal of High Energy Physics
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On the strength of the U A (1) anomaly at the chiral phase transition in N f = 2 QCD

2016

We study the thermal transition of QCD with two degenerate light flavours by lattice simulations using $O(a)$-improved Wilson quarks. Temperature scans are performed at a fixed value of $N_t = (aT)^{-1}=16$, where $a$ is the lattice spacing and $T$ the temperature, at three fixed zero-temperature pion masses between 200 MeV and 540 MeV. In this range we find that the transition is consistent with a broad crossover. As a probe of the restoration of chiral symmetry, we study the static screening spectrum. We observe a degeneracy between the transverse isovector vector and axial-vector channels starting from the transition temperature. Particularly striking is the strong reduction of the split…

Nuclear and High Energy PhysicsNuclear TheorySpontaneous symmetry breakingHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)PionHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsMass screeningPhysicsQuantum chromodynamicsIsovectorCondensed matter physics010308 nuclear & particles physicsTransition temperatureMESON SCREENING MASSES; HIGH-TEMPERATURE PHASE; QUARK-GLUON PLASMA; LATTICE QCD; WILSON FERMIONS; HADRONIC SPECTRUM; O(A) IMPROVEMENT; U(1)(A) SYMMETRY; GAUGE-THEORIES; STRANGE QUARK; Global Symmetries; Lattice QCD; Phase Diagram of QCD; Spontaneous Symmetry BreakingHigh Energy Physics - Lattice (hep-lat)ddc:530Lattice QCD530 PhysikPseudoscalarHigh Energy Physics - Phenomenology
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A strategy to study the role of the charm quark in explaining the Delta{I}=1/2 rule

2004

We present a strategy designed to separate several possible origins of the well-known enhancement of the Delta{I}=1/2 amplitude in non-leptonic kaon decays. In particular, we seek to disentangle the contribution of physics at the typical QCD scale (soft-gluon exchange) from the effects at the scale of the charm quark mass. This is achieved by considering QCD with an unphysically light charm quark, so that the theory possesses an approximate SU(4)_L x SU(4)_R chiral symmetry. By computing the relevant operator matrix elements and monitoring their values as the charm quark mass departs from the SU(4)-symmetric situation, the role of the charm quark can be assessed. We study the influence of t…

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeLattice (group)FOS: Physical sciencesScale (descriptive set theory)weak decaysCharm quarkHigh Energy Physics - Phenomenology (hep-ph)lattice QCDHigh Energy Physics - Latticefield theory gauge theory lattice kaon decayskaon physicschiral lagrangiansLimit (mathematics)Quantum chromodynamicsPhysicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - PhenomenologyAmplitudeOperator matrixHigh Energy Physics::Experiment
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High-precision determination of the $K_{e3}$ radiative corrections

2021

We report a high-precision calculation of the Standard Model electroweak radiative corrections in the $K\to \pi e^+\nu(\gamma)$ decay as a part of the combined theory effort to understand the existing anomaly in the determinations of $V_{us}$. Our new analysis features a chiral resummation of the large infrared-singular terms in the radiative corrections and a well-under-control strong interaction uncertainty based on the most recent lattice QCD inputs. While being consistent with the current state-of-the-art results obtained from chiral perturbation theory, we reduce the existing theory uncertainty from $10^{-3}$ to $10^{-4}$. Our result suggests that the Standard Model electroweak effects…

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear TheoryQC1-999Strong interactionFOS: Physical sciences01 natural sciencesStandard ModelHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesRadiative transferddc:530ResummationNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsPhysicsElectroweak interactionHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)Lattice QCDHigh Energy Physics - PhenomenologyAnomaly (physics)
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New method for calculating electromagnetic effects in semileptonic beta-decays of mesons

2020

We construct several classes of hadronic matrix elements and relate them to the low-energy constants in Chiral Perturbation Theory that describe the electromagnetic effects in the semileptonic beta decay of the pion and the kaon. We propose to calculate them using lattice QCD, and argue that such a calculation will make an immediate impact to a number of interesting topics at the precision frontier, including the outstanding anomalies in $|V_{us}|$ and the top-row Cabibbo-Kobayashi-Maskawa matrix unitarity.

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryelectromagnetic [effect]MesonNuclear TheoryHigh Energy Physics::LatticeHadronFOS: Physical scienceschiral [perturbation theory]anomalyLattice QCD01 natural sciences530High Energy Physics - ExperimentNuclear Theory (nucl-th)Matrix (mathematics)High Energy Physics - Experiment (hep-ex)Kaon PhysicsPionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciencesBeta (velocity)lcsh:Nuclear and particle physics. Atomic energy. Radioactivityddc:530Precision QEDNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysicsUnitarity010308 nuclear & particles physicsComputer Science::Information RetrievalHigh Energy Physics - Lattice (hep-lat)High Energy Physics::Phenomenologysemileptonic decay [meson]lattice field theorysemileptonic decay [pi]Lattice QCDHigh Energy Physics - PhenomenologyChiral Lagrangianslcsh:QC770-798High Energy Physics::Experimentunitarity [CKM matrix]
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Scalar spectrum in a graviton soft wall model

2020

In this study we present a unified phenomenological analysis of the scalar glueball and scalar meson spectra within an AdS/QCD framework in the bottom up approach. For this purpose we generalize the recently developed graviton soft-wall (GSW) model, which has shown an excellent agreement with the lattice QCD glueball spectrum, to a description of glueballs and mesons with a unique energy scale. In this scheme, dilatonic effects, are incorporated in the metric as a deformation of the AdS space. We apply the model also to the heavy meson spectra with success. We obtain quadratic mass equations for all scalar mesons while the glueballs satisfy an almost linear mass equation. Besides their spec…

Nuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryHigh Energy Physics::LatticeScalar (mathematics)FOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Spectrum0103 physical sciencesAdS/CFT010306 general physicsScalar mesonQuantum chromodynamicsPhysics010308 nuclear & particles physicsGlueballHigh Energy Physics::PhenomenologyGravitonLattice QCDMesonMass formulaHigh Energy Physics - PhenomenologyGlueballHigh Energy Physics::Experiment
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Nature of the light scalar mesons

2005

Despite the apparent simplicity of meson spectroscopy, light scalar mesons cannot be accommodated in the usual $q\bar q$ structure. We study the description of the scalar mesons below 2 GeV in terms of the mixing of a chiral nonet of tetraquarks with conventional $q\bar q$ states. A strong diquark-antidiquark component is found for several states. The consideration of a glueball as dictated by quenched lattice QCD drives a coherent picture of the isoscalar mesons.

Nuclear and High Energy PhysicsParticle physicsMesonNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]IsoscalarHigh Energy Physics::Latticemeson massquark confinementLattice field theoryNuclear TheoryFOS: Physical sciencessparticles01 natural sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesquantum chromodynamics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysics010308 nuclear & particles physicsGlueballHigh Energy Physics::PhenomenologyScalar (physics)lattice field theory12.39.-x 12.38.-tFísicaLattice QCDDiquarkHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimentchiral symmetries
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Numerical exploration of three relativistic particles in a finite volume including two-particle resonances and bound states

2019

In this work, we use an extension of the quantization condition, given in Ref. [1], to numerically explore the finite-volume spectrum of three relativistic particles, in the case that two-particle subsets are either resonant or bound. The original form of the relativistic three-particle quantization condition was derived under a technical assumption on the two-particle K matrix that required the absence of two-particle bound states or narrow two-particle resonances. Here we describe how this restriction can be lifted in a simple way using the freedom in the definition of the K-matrix-like quantity that enters the quantization condition. With this in hand, we extend previous numerical studie…

Nuclear and High Energy Physicsnucl-thNuclear TheoryAtomic Physics (physics.atom-ph)Other Fields of Physicshep-latFOS: Physical sciencesLattice QCDphysics.atom-ph01 natural sciencesPhysics - Atomic PhysicsRelativistic particleNuclear Theory (nucl-th)Quantization (physics)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanics0103 physical sciencesBound statelcsh:Nuclear and particle physics. Atomic energy. Radioactivitycond-mat.stat-mech010306 general physicsScattering AmplitudesCondensed Matter - Statistical MechanicsParticle Physics - PhenomenologyPhysicsFinite volume methodStatistical Mechanics (cond-mat.stat-mech)010308 nuclear & particles physicsScatteringHigh Energy Physics - Lattice (hep-lat)hep-phParticle Physics - LatticeLattice QCDScattering amplitudeHigh Energy Physics - PhenomenologyAmplitudeNuclear Physics - Theorylcsh:QC770-798
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