Search results for "PARTICLE PHYSICS"

showing 10 items of 6826 documents

Test of the heavy quark-light diquark approximation for baryons with a heavy quark

2008

We check a commonly used approximation in which a baryon with a heavy quark is described as a heavy quark-light diquark system. The heavy quark influences the diquark internal motion reducing the average distance between the two light quarks. Besides, we show how the average distance between the heavy quark and any of the light quarks, and that between the heavy quark and the center of mass of the light diquark, are smaller than the distance between the two light quarks, which seems to contradict the heavy quark-light diquark picture. This latter result is in agreement with expectations from QCD sum rules and lattice QCD calculations. Our results also show that the diquark approximations pr…

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsQCD sum rulesParticle physicsNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaLattice QCDNuclear Theory (nucl-th)DiquarkNuclear physicsBaryonCharmed baryonsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentCenter of massNuclear Experiment
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Up, down, strange and charm quark masses withNf=2+1+1twisted mass lattice QCD

2014

Abstract We present a lattice QCD calculation of the up, down, strange and charm quark masses performed using the gauge configurations produced by the European Twisted Mass Collaboration with N f = 2 + 1 + 1 dynamical quarks, which include in the sea, besides two light mass degenerate quarks, also the strange and charm quarks with masses close to their physical values. The simulations are based on a unitary setup for the two light quarks and on a mixed action approach for the strange and charm quarks. The analysis uses data at three values of the lattice spacing and pion masses in the range 210 – 450 MeV , allowing for accurate continuum limit and controlled chiral extrapolation. The quark …

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsStrange quarkParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryLattice QCD7. Clean energySigma baryonCharm quarkNuclear physicsPionUp quarkHigh Energy Physics::ExperimentNuclear ExperimentNuclear Physics B
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Top-Quark Charge Asymmetry with a Jet Handle

2012

Pairs of top and antitop quarks are produced at the LHC to a large extent in association with a hard jet. We investigate the charge asymmetry in top pair + jet production in quantum chromodynamics (QCD) and with additional massive color-octet vector bosons. The total charge asymmetry at the LHC is suppressed by the large charge-symmetric background from gluon-gluon fusion. We show to what extent the asymmetry can be enhanced by suitable phase space cuts and, in particular, elaborate on the kinematics of the hard jet in the top pair + jet final state. We demonstrate that in QCD, the asymmetry amounts to -1.5% for central jets without an excessive reduction of the cross section. By applying a…

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsTop quarkParticle physicsmedia_common.quotation_subjectHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesCharge (physics)Jet (particle physics)AsymmetryHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Production (computer science)High Energy Physics::Experimentmedia_commonBoson
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Kl3Semileptonic Form Factor from (2+1)-Flavor Lattice QCD

2008

We present the first results for the ${K}_{l3}$ form factor from simulations with $2+1$ flavors of dynamical domain wall quarks. Combining our result, namely, ${f}_{+}(0)=0.964(5)$ with the latest experimental results for ${K}_{l3}$ decays leads to $|{V}_{us}|=0.2249(14)$, reducing the uncertaintity in this important parameter. For the $O({p}^{6})$ term in the chiral expansion we obtain $\ensuremath{\Delta}f=\ensuremath{-}0.013(5)$.

QuarkPhysicsQuantum chromodynamicsParticle physics010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixLattice field theoryForm factor (quantum field theory)General Physics and AstronomyLattice QCD01 natural sciencesDomain wall (magnetism)Lattice gauge theory0103 physical sciences010306 general physicsPhysical Review Letters
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Quark and gluon form factors to four-loop order in QCD: TheNf3contributions

2017

We calculate the four-loop massless QCD corrections with three closed quark lines to quark and gluon form factors. We apply a novel integration by parts algorithm based on modular arithmetic and compute all relevant master integrals for arbitrary values of the space-time dimension. This is the first calculation of a gluon form factor at this perturbative order in QCD.

QuarkPhysicsQuantum chromodynamicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyQCD vacuumForm factor (quantum field theory)Jet (particle physics)01 natural sciencesBottom quarkGluonMassless particle0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsPhysical Review D
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Kaon Physics: Theory Overview

2012

Kaon decays have played a key role in the construction of the Standard Model and continue to be an important testing ground of the electroweak flavour theory. They can provide new signals of CP-violation phenomena and, perhaps, a window into physics beyond the Standard Model. The interplay of long-distance QCD effects in strangeness-changing transitions can be analyzed, combining the short-distance Operator Product Expansion with Chiral Perturbation Theory techniques. A brief overview is presented, focusing on a few selected decay modes. A more detailed and comprehensive review can be found in arXiv:1107.6001.

QuarkPhysicsQuantum chromodynamicsParticle physicsChiral perturbation theoryPhysics beyond the Standard ModelElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesHigh Energy Physics - ExperimentStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)CP violationHigh Energy Physics::ExperimentOperator product expansion
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K--pipi amplitudes from lattice QCD with a light charm quark.

2006

4 pages, 1 figure.-- PACS nrs.: 12.38.Gc, 13.25.Es, 11.30.Rd.-- ISI Article Identifier: 000244420700019.-- ArXiv pre-print available at: http://arxiv.org/abs/hep-ph/0607220

QuarkPhysicsQuantum chromodynamicsParticle physicsChiral perturbation theoryTo-leading orderHigh Energy Physics::LatticeLattice field theoryHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyFísica[PACS] Lattice QCD calculations[PACS] Chiral symmetries in particles and fieldsQuenched approximationLattice QCD[PACS] Hadronic decays of K mesonsCharm quarkHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticePionChiral perturbation theoryHigh Energy Physics::ExperimentWeak interactionsWilson fermionsPhysical review letters
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Gluon contribution to hadronicJψproduction

1978

Using the recent CERN and Fermilab measurements for J/ψ production by π±, K±, p and p beams we show, within the framework of QCD, that only a combined version of light quark qq→cc fusion and gluon gg→cc fusion mechanisms can account for the various total cross section beam ratios as well as for the observed xF‐distributions.

QuarkPhysicsQuantum chromodynamicsParticle physicsMesonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyQuark modelHadronElementary particleGluonNuclear physicsPhysics::Accelerator PhysicsNuclear fusionHigh Energy Physics::ExperimentPhysical Review D
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Unified QCD determination of all pseudoscalar leptonic decay constants

1992

Leptonic decay constants of all pseudoscalar mesons are determined in QCD by means of a new QCD sum-rule method. In the light meson and heavy quark limit the results are very similar and also agree with the well-known PCAC and scaling predictions respectively. The corrections to light meson pole dominance are generally small while those to the heavy quark limit are found to be sensitive to the binding energy (i.e. meson and quark mass differences). For standard values of quark masses we obtainfπ=132 MeV,fk=161 MeV,fB=128±28 MeV,fD=175±13 MeV,fBs=144±30 MeV andfDs=193±12 MeV.

QuarkPhysicsQuantum chromodynamicsParticle physicsPhysics and Astronomy (miscellaneous)MesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyBinding energyElementary particleBottom quarkNuclear physicsPseudoscalarHigh Energy Physics::ExperimentQuantum field theoryNuclear ExperimentEngineering (miscellaneous)Zeitschrift für Physik C Particles and Fields
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Charmonium dissociation and heavy quark transport in hot quenched lattice QCD

2012

We study the properties of charmonium states at finite temperature in quenched lattice QCD on large and fine isotropic lattices. We perform a detailed analysis of charmonium correlation and spectral functions both below and above Tc. Our analysis suggests that the S wave states disappear at about 1.5 Tc. The charm diffusion coefficient is estimated and found to be approximately 1/{\pi}T at 1.5Tc {\leq} T {\leq} 3Tc.

QuarkPhysicsQuenchingParticle physicsSpectral representationNuclear TheoryPhysicsQC1-999High Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyLattice field theoryIsotropyFOS: Physical sciencesLattice QCDDissociation (chemistry)Nuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)S-waveHigh Energy Physics::ExperimentEPJ Web of Conferences
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