Search results for "High Energy Physics - Lattice"

showing 10 items of 466 documents

Dynamical twisted mass fermions with light quarks: simulation and analysis details

2008

In a recent paper [hep-lat/0701012] we presented precise lattice QCD results of our European Twisted Mass Collaboration (ETMC). They were obtained by employing two mass-degenerate flavours of twisted mass fermions at maximal twist. In the present paper we give details on our simulations and the computation of physical observables. In particular, we discuss the problem of tuning to maximal twist, the techniques we have used to compute correlators and error estimates. In addition, we provide more information on the algorithm used, the autocorrelation times and scale determination, the evaluation of disconnected contributions and the description of our data by means of chiral perturbation theo…

QuarkParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeLattice field theoryGeneral Physics and AstronomyFOS: Physical sciencesHybrid Monte Carlo algorithmLattice QCD01 natural sciencesRenormalizationStochastic quark propagatorsTheoretical physicsHigh Energy Physics - LatticeLattice gauge theory0103 physical sciencesHybrid Monte Carlo algorithm; Lattice gauge theory; Lattice QCD; Stochastic quark propagators010306 general physicsPhysicsQuantum chromodynamics010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics - Lattice (hep-lat)FísicaLattice QCDFermionSettore FIS/02 - Fisica Teorica Modelli e Metodi MatematiciLattice gauge theoryHardware and Architectureddc:004
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Electromagnetic form factors of spin 1/2 doubly charmed baryons

2018

We study the electromagnetic form factors of the doubly charmed baryons, using covariant chiral perturbation theory within the extended on-mass-shell (EOMS) scheme. Vector-meson contributions are also taken into account. We present results for the baryon magnetic moments, charge and magnetic radii. While some of the chiral Lagrangian parameters could be set to values determined in previous works, the available lattice results for $\Xi_{cc}^+$ and $\Omega_{cc}^+$ only allow for robust constraints on the low-energy constant (LEC) combination, $c_{89}(=-\frac{1}{3}c_8+4c_9)$. The couplings of the doubly charmed baryons to the vector mesons have been estimated assuming the Okubo--Zweig--Iizuka …

QuarkParticle physicsChiral perturbation theoryMesonHeavy baryon chiral perturbation theoryHigh Energy Physics::LatticeLattice field theoryNuclear TheoryFOS: Physical sciencesComputer Science::Digital Libraries01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNuclear ExperimentPhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)Charmed baryonsBaryonHigh Energy Physics - Phenomenology
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Cosmic QCD Epoch at Nonvanishing Lepton Asymmetry

2018

We investigate how a lepton asymmetry impacts the cosmic trajectory in the QCD phase diagram. We study the evolution of chemical potentials during the QCD epoch of the early Universe using susceptibilities from lattice QCD to interpolate between an ideal quark gas and an ideal hadron resonance gas. The lepton asymmetry affects the evolution of all chemical potentials. The standard cosmic trajectory is obtained assuming tiny lepton and baryon asymmetries. For larger lepton asymmetry, the charge chemical potential exceeds the baryon chemical potential before pion annihilation.

QuarkParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)media_common.quotation_subjectHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesGeneral Physics and AstronomyAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesAsymmetryHigh Energy Physics - Phenomenology (hep-ph)PionHigh Energy Physics - Lattice0103 physical sciences010306 general physicsmedia_commonQuantum chromodynamicsPhysics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyLattice QCDUniverseBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentLeptonAstrophysics - Cosmology and Nongalactic Astrophysics
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Joint lattice QCD–dispersion theory analysis confirms the quark-mixing top-row unitarity deficit

2020

Recently, the first ever lattice computation of the $\gamma W$-box radiative correction to the rate of the semileptonic pion decay allowed for a reduction of the theory uncertainty of that rate by a factor of $\sim3$. A recent dispersion evaluation of the $\gamma W$-box correction on the neutron also led to a significant reduction of the theory uncertainty, but shifted the value of $V_{ud}$ extracted from the neutron and superallowed nuclear $\beta$ decay, resulting in a deficit of the CKM unitarity in the top row. A direct lattice computation of the $\gamma W$-box correction for the neutron decay would provide an independent cross-check for this result but is very challenging. Before those…

QuarkParticle physicsNuclear TheoryComputationAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesComputer Science::Digital Libraries01 natural sciences530High Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)PionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeLattice (order)0103 physical sciencesRadiative transferddc:530NeutronNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysicsUnitarity010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Lattice QCDHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentPhysical Review D
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Decay constants of B-mesons from non-perturbative HQET with two light dynamical quarks

2014

We present a computation of B-meson decay constants from lattice QCD simulations within the framework of Heavy Quark Effective Theory for the b-quark. The next-to-leading order corrections in the HQET expansion are included non-perturbatively. Based on Nf=2 gauge field ensembles, covering three lattice spacings a (0.08-0.05)fm and pion masses down to 190MeV, a variational method for extracting hadronic matrix elements is used to keep systematic errors under control. In addition we perform a careful autocorrelation analysis in the extrapolation to the continuum and to the physical pion mass limits. Our final results read fB=186(13)MeV, fBs=224(14)MeV and fBs/fB=1.203(65). A comparison with o…

QuarkParticle physicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHadronLattice field theoryNuclear Theoryhep-latFOS: Physical sciencesLattice QCD01 natural sciencesNuclear physicsRenormalizationPionHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesMeson decayB mesonddc:530010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsHeavy Quark Effective Theory010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics - Lattice (hep-lat)High Energy Physics::Phenomenologyhep-phLattice QCDHigh Energy Physics - PhenomenologyBottom quarks[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experiment
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B-physics from Nf=2 tmQCD: the Standard Model and beyond

2013

Carrasco, Nuria et al.

QuarkParticle physicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesbottom quark mass01 natural sciencesBottom quarkStandard ModelLattice constantPionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciencesContinuum (set theory)010306 general physicsNuclear ExperimentPhysicsUnitarity[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaParticle Physics - LatticeLattice QCDB-physicsSM and beyondSettore FIS/02 - Fisica Teorica Modelli e Metodi MatematiciHigh Energy Physics - PhenomenologyB-physics; bottom quark mass; B-meson mixing; SM and beyond[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]B-meson mixingHigh Energy Physics::Experiment
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Bridging a gap between continuum-QCD and ab initio predictions of hadron observables

2015

Within contemporary hadron physics there are two common methods for determining the momentum-dependence of the interaction between quarks: the top-down approach, which works toward an ab initio computation of the interaction via direct analysis of the gauge-sector gap equations; and the bottom-up scheme, which aims to infer the interaction by fitting data within a well-defined truncation of those equations in the matter sector that are relevant to bound-state properties. We unite these two approaches by demonstrating that the renormalisation-group-invariant running-interaction predicted by contemporary analyses of QCD's gauge sector coincides with that required in order to describe ground-s…

QuarkParticle physicsNuclear and High Energy PhysicsNuclear TheoryHigh Energy Physics::LatticeGribov copiesHadronAb initioFOS: Physical sciencesNuclear Theory (nucl-th)High Energy Physics::TheoryHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Hadron physicsFragmentationBound stateNuclear Experiment (nucl-ex)Nuclear ExperimentQuantum chromodynamicsPhysicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaObservablelcsh:QC1-999High Energy Physics - PhenomenologyDyson–Schwinger equationsDynamical chiral symmetry breakingPreprintlcsh:PhysicsConfinementPhysics Letters B
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The rate of photon production in the quark-gluon plasma from lattice QCD

2020

We calculate the thermal rate of real-photon production in the quark-gluon plasma at a temperature of $T=254$ MeV using lattice QCD. The calculation is based on the difference between the spatially transverse and longitudinal parts of the polarization tensor, which has the advantage of falling off rapidly at large frequencies. We obtain this linear combination in the time-momentum representation from lattice QCD with two flavors of quarks in the continuum limit with a precision of about two parts per mille. Applying a theoretically motivated fit ansatz for the associated spectral function, we obtain values for the photon rate that are in line with QCD weak-coupling calculations; for photon …

QuarkParticle physicsPhotonNuclear Theorynucl-thHigh Energy Physics::LatticePhoton Production RateFOS: Physical scienceshep-latLattice QCD7. Clean energy01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsLinear combinationAnsatzParticle Physics - PhenomenologyQuantum chromodynamicsPhysics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::Phenomenologyhep-phParticle Physics - LatticeLattice QCDPolarization (waves)3. Good healthHigh Energy Physics - PhenomenologyNuclear Physics - TheoryQuark–gluon plasmaQuark-Gluon PlasmaHigh Energy Physics::Experiment
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Spectrum of fully-heavy tetraquarks from a diquark+antidiquark perspective

2019

Using a relativized diquark model Hamiltonian, we calculate the masses of $J^{PC}=0^{++}$ ground-state tetraquarks in the following systems: $b s \bar b \bar s$, $bb \bar n \bar n$ ($n=u, d$), $bb \bar s \bar s$, $cc\bar c \bar c$, $b b \bar b \bar b$, $b c\bar b \bar c$ and $b b \bar c \bar c$. We also compute extensive spectra for the fully-heavy quark flavour combinations. Finally, as a test of the diquark model approach, we compute the masses of fully-heavy baryons in the diquark model. Our results may be compared soon to the forthcoming experimental data for fully-heavy three-quark systems.

QuarkParticle physicsPhysics and Astronomy (miscellaneous)Nuclear TheoryHigh Energy Physics::LatticeNuclear TheoryFOS: Physical scienceslcsh:AstrophysicshiukkasfysiikkaHigh Energy Physics - ExperimentNuclear Theory (nucl-th)symbols.namesakeHigh Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)lcsh:QB460-466lcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclear Experiment (nucl-ex)Engineering (miscellaneous)Nuclear theoryNuclear ExperimentPhysicstheoretical physicskvarkitHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)DiquarkBaryonHigh Energy Physics - Phenomenologysymbolslcsh:QC770-798High Energy Physics::ExperimentHamiltonian (quantum mechanics)European Physical Journal
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The hadronic contribution to the running of the electromagnetic coupling and the electroweak mixing angle

2019

37th International Symposium on Lattice Field Theory, Wuhan, China, 16 Jun 2019 - 22 Jun 2019; PoS(LATTICE 2019)010 (2019).

QuarkParticle physicsneutral currentclover [fermion]High Energy Physics::LatticeHadronstandard modelLattice (group)hep-latWilson [quark]FOS: Physical sciencesLattice QCDelectromagnetic [current]nonperturbativeStandard Modelenergy dependenceHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)quantum chromodynamicshadronic [vacuum polarization]mixingVacuum polarizationcontinuum limitnumerical calculationsParticle Physics - PhenomenologylatticePhysicsElectroweak interactionHigh Energy Physics - Lattice (hep-lat)lattice field theoryflavor: 3 [quark]hep-phParticle Physics - LatticeFermionmass dependence [quark]High Energy Physics - Phenomenologyelectromagnetic [coupling]mixing angle [electroweak interaction]Energy (signal processing)
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